Showing 50 of 6089 results
The cross section asymmetry Sigma has been measured for the photoproduction of pi0-mesons off protons, using polarized photons in the energy range Eg = 0.5 - 1.1 GeV. The CM angular coverage is Theta = 85 - 125 deg with energy and angle steps of 25 MeV and 5 deg, respectively. The obtained Sigma data, which cover the second and third resonance regions, are compared with existing experimental data and recent phenomenological analyses. The influence of these measurements on such analyses is also considered.
Axis error includes +- 3/3 contribution (Due to accuracy of the linear polarization calculations).
Axis error includes +- 3/3 contribution (Due to accuracy of the linear polarization calculations).
Axis error includes +- 3/3 contribution (Due to accuracy of the linear polarization calculations).
Axis error includes +- 3/3 contribution (Due to accuracy of the linear polarization calculations).
Axis error includes +- 3/3 contribution (Due to accuracy of the linear polarization calculations).
Axis error includes +- 3/3 contribution (Due to accuracy of the linear polarization calculations).
Axis error includes +- 3/3 contribution (Due to accuracy of the linear polarization calculations).
Axis error includes +- 3/3 contribution (Due to accuracy of the linear polarization calculations).
Axis error includes +- 3/3 contribution (Due to accuracy of the linear polarization calculations).
The analyzing power,$A_{oono}$, and the polarization transfer observables$K_{onno}$,$K_{os''so}$
Position 'A' (see text for explanation).
Position 'A' (see text for explanation).
Position 'A' (see text for explanation).
Position 'A' (see text for explanation).
Position 'A' (see text for explanation).
Position 'B' (see text for explanation).
Position 'B' (see text for explanation).
Position 'B' (see text for explanation).
Position 'B' (see text for explanation).
Position 'B' (see text for explanation).
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The strong coupling constant, αs, has been determined in hadronic decays of theZ0 resonance, using measurements of seven observables relating to global event shapes, energy correlatio
Data corrected for finite acceptance and resolution of the detector and for intial state photon radiation. No corrections for hadronic effects are applied.. Errors include statistical and systematic uncertainties, added in quadrature.
Data corrected for finite acceptance and resolution of the detector and for intial state photon radiation. No corrections for hadronic effects are applied.. Errors include statistical and systematic uncertainties, added in quadrature.
Data corrected for finite acceptance and resolution of the detector and for intial state photon radiation. No corrections for hadronic effects are applied.. Errors include statistical and systematic uncertainties, added in quadrature.
Data corrected for finite acceptance and resolution of the detector and for intial state photon radiation. No corrections for hadronic effects are applied.. Errors include statistical and systematic uncertainties, added in quadrature.
Data corrected for finite acceptance and resolution of the detector and for intial state photon radiation. No corrections for hadronic effects are applied.. Errors include statistical and systematic uncertainties, added in quadrature.
Data corrected for finite acceptance and resolution of the detector and for intial state photon radiation. No corrections for hadronic effects are applied.. Errors include statistical and systematic uncertainties, added in quadrature.. YCUT is the cut off value used to define the jets in this case using the 'Durham' scheme.
Data corrected for finite acceptance and resolution of the detector and for intial state photon radiation. No corrections for hadronic effects are applied.. Errors include statistical and systematic uncertainties, added in quadrature.. YCUT is the cut off value used to define the jets in this case using the 'Durham' scheme.. D2 is the differential jet rate.
A polarized proton beam extracted from SATURNE II and the Saclay polarized proton target were used to measure the rescattering observables$K_{onno}$and
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An experimental investigation of the structure of identified quark and gluon jets is presented. Observables related to both the global and internal structure of jets are measured; this allows for test
The measured jet broadening distributions (B) in quark and gluon jets seperately.
Measured distributions of -LN(Y2), where Y2 is the differential one-subjet rate, that is the value of the subjet scale parameter where 2 jets appear from the single jet.
The mean subjet multiplicity (-1) for gluon jets and quark jets for different values of the subject resolution parameter Y0.
The standard deviation (DISPERSION) of the subject multiplicity for gluon jets and quark jets for different values of the subject resolution parameter Y0.
The ratio of the multiplicities and their standard deviations for the subject in quark and gluon jets as a function of the subject resolution parameter Y0.
The measured fragmentation function for charged particles within quark and gluon jets.
A double scattering experiment, performed at the Paul-Scherrer-Institut (PSI), has measured a large variety of spin observables for free np elastic scattering from 260 to 535 MeV in the c.m. angle ran
Measurements of DNN with statistical errors only.
Measurements of DSL with statistical errors only.
Measurements of DSS with statistical errors only.
Measurements of KNN with statistical errors only.
Measurements of KSL with statistical errors only.
Measurements of KSS with statistical errors only.
Measurements of the triple spin parameter NNLL with statistical errors only.
Measurements of the triple spin parameter NSLN with statistical errors only.
Measurements of the triple spin parameter NSNS with statistical errors only.
Measurements of the triple spin parameter NSSN with statistical errors only.
Polarization transfer observables in π + d elastic scattering have been measured for the first time. Four polarization transfer parameters were determined at pion energies T π =134 MeV and 180 MeV at scattering angles θ π ,C.M. between 100° and 140° using a deuteron target polarized perpendicular to the scattering plane and a deuteron tensor polarimeter. The data are compared to different predictions from the SAID phase shift analysis and Faddeev calculations.
Systematic and statistical errors are added in quadrature.
Systematic and statistical errors are added in quadrature.
We report measurements of spin correlations and analyzing powers in He→3(p→, 2p) and He→3(p→, pn) quasielastic scattering as a function of momentum transfer and missing momentum at 197 MeV using a polarized internal target at the Indiana University Cyclotron Facility Cooler Ring. At sufficiently high momentum transfer we find He→3(p→, pn) spin observables are in good agreement with free p−n scattering observables, and therefore that He→3 can serve as a good polarized neutron target. The extracted polarizations of nucleons in He→3 at low missing momentum are consistent with Faddeev calculations.
QUASIELASTIC SCATTERING.
Jet substructure quantities are measured using jets groomed with the soft-drop grooming procedure in dijet events from 32.9 fb$^{-1}$ of $pp$ collisions collected with the ATLAS detector at $\sqrt{s} = 13$ TeV. These observables are sensitive to a wide range of QCD phenomena. Some observables, such as the jet mass and opening angle between the two subjets which pass the soft-drop condition, can be described by a high-order (resummed) series in the strong coupling constant $\alpha_S$. Other observables, such as the momentum sharing between the two subjets, are nearly independent of $\alpha_S$. These observables can be constructed using all interacting particles or using only charged particles reconstructed in the inner tracking detectors. Track-based versions of these observables are not collinear safe, but are measured more precisely, and universal non-perturbative functions can absorb the collinear singularities. The unfolded data are directly compared with QCD calculations and hadron-level Monte Carlo simulations. The measurements are performed in different pseudorapidity regions, which are then used to extract quark and gluon jet shapes using the predicted quark and gluon fractions in each region. All of the parton shower and analytical calculations provide an excellent description of the data in most regions of phase space.
Data from Fig 6a. The unfolded all-particle $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from Fig 6a. The unfolded all-particle $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from Fig 6b. The unfolded charged-particle $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from Fig 6b. The unfolded charged-particle $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from Fig 6c. The unfolded all-particle $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from Fig 6c. The unfolded all-particle $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from Fig 6d. The unfolded charged-particle $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from Fig 6d. The unfolded charged-particle $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from Fig 6e. The unfolded $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from Fig 6e. The unfolded $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from Fig 6f. The unfolded charged-particle $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from Fig 6f. The unfolded charged-particle $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from Fig 7a. The unfolded all-particle $z_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 10 bins corresponds to one $p_T$ bin in (300, 400, 600, 800, 1000, infinity) and 10 evenly spaced bins in $z_g$ from 0.0 to 0.5.
Data from Fig 7a. The unfolded all-particle $z_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 10 bins corresponds to one $p_T$ bin in (300, 400, 600, 800, 1000, infinity) and 10 evenly spaced bins in $z_g$ from 0.0 to 0.5.
Data from Fig 7b. The unfolded all-particle $z_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 10 bins corresponds to one $p_T$ bin in (300, 400, 600, 800, 1000, infinity) and 10 evenly spaced bins in $z_g$ from 0.0 to 0.5.
Data from Fig 7b. The unfolded all-particle $z_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 10 bins corresponds to one $p_T$ bin in (300, 400, 600, 800, 1000, infinity) and 10 evenly spaced bins in $z_g$ from 0.0 to 0.5.
Data from Fig 7c. The unfolded all-particle $z_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 10 bins corresponds to one $p_T$ bin in (300, 400, 600, 800, 1000, infinity) and 10 evenly spaced bins in $z_g$ from 0.0 to 0.5.
Data from Fig 7c. The unfolded all-particle $z_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 10 bins corresponds to one $p_T$ bin in (300, 400, 600, 800, 1000, infinity) and 10 evenly spaced bins in $z_g$ from 0.0 to 0.5.
Data from Fig 7d. The unfolded all-particle $z_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 10 bins corresponds to one $p_T$ bin in (300, 400, 600, 800, 1000, infinity) and 10 evenly spaced bins in $z_g$ from 0.0 to 0.5.
Data from Fig 7d. The unfolded all-particle $z_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 10 bins corresponds to one $p_T$ bin in (300, 400, 600, 800, 1000, infinity) and 10 evenly spaced bins in $z_g$ from 0.0 to 0.5.
Data from Fig 7e. The unfolded all-particle $z_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 10 bins corresponds to one $p_T$ bin in (300, 400, 600, 800, 1000, infinity) and 10 evenly spaced bins in $z_g$ from 0.0 to 0.5.
Data from Fig 7e. The unfolded all-particle $z_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 10 bins corresponds to one $p_T$ bin in (300, 400, 600, 800, 1000, infinity) and 10 evenly spaced bins in $z_g$ from 0.0 to 0.5.
Data from Fig 7f. The unfolded all-particle $z_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 10 bins corresponds to one $p_T$ bin in (300, 400, 600, 800, 1000, infinity) and 10 evenly spaced bins in $z_g$ from 0.0 to 0.5.
Data from Fig 7f. The unfolded all-particle $z_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 10 bins corresponds to one $p_T$ bin in (300, 400, 600, 800, 1000, infinity) and 10 evenly spaced bins in $z_g$ from 0.0 to 0.5.
Data from Fig 8a. The unfolded all-particle $R_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from Fig 8a. The unfolded all-particle $R_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from Fig 8b. The unfolded all-particle $R_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from Fig 8b. The unfolded all-particle $R_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from Fig 8c. The unfolded all-particle $R_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from Fig 8c. The unfolded all-particle $R_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from Fig 8d. The unfolded all-particle $R_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from Fig 8d. The unfolded all-particle $R_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from Fig 8e. The unfolded all-particle $R_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from Fig 8e. The unfolded all-particle $R_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from Fig 8f. The unfolded all-particle $R_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from Fig 8f. The unfolded all-particle $R_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from Fig 14a. The unfolded all-particle $log_{10}(\rho^2)$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from Fig 14a. The unfolded all-particle $log_{10}(\rho^2)$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from Fig 14b. The unfolded charged-particle $log_{10}(\rho^2)$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from Fig 14b. The unfolded charged-particle $log_{10}(\rho^2)$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from FigAux 4b. The unfolded all-particle $log_{10}(\rho^2)$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from FigAux 4b. The unfolded all-particle $log_{10}(\rho^2)$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from FigAux 21b. The unfolded charged-particle $log_{10}(\rho^2)$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from FigAux 21b. The unfolded charged-particle $log_{10}(\rho^2)$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from FigAux 5a. The unfolded $log_{10}(\rho^2)$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from FigAux 5a. The unfolded $log_{10}(\rho^2)$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from FigAux 5b. The unfolded charged-particle $log_{10}(\rho^2)$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from FigAux 5b. The unfolded charged-particle $log_{10}(\rho^2)$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from Fig 14c. The unfolded all-particle $z_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from Fig 14c. The unfolded all-particle $z_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from Fig 14d. The unfolded all-particle $z_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from Fig 14d. The unfolded all-particle $z_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 4c. The unfolded all-particle $z_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 4c. The unfolded all-particle $z_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 4d. The unfolded all-particle $z_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 4d. The unfolded all-particle $z_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 5c. The unfolded all-particle $z_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 5c. The unfolded all-particle $z_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 5d. The unfolded all-particle $z_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 5d. The unfolded all-particle $z_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from Fig 14e. The unfolded all-particle $R_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from Fig 14e. The unfolded all-particle $R_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from Fig 14f. The unfolded all-particle $R_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from Fig 14f. The unfolded all-particle $R_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 4e. The unfolded all-particle $R_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 4e. The unfolded all-particle $R_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 4f. The unfolded all-particle $R_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 4f. The unfolded all-particle $R_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 5e. The unfolded all-particle $R_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 5e. The unfolded all-particle $R_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 5f. The unfolded all-particle $R_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 5f. The unfolded all-particle $R_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from Fig 14a. The unfolded all-particle $log_{10}(\rho^2)$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from Fig 14a. The unfolded all-particle $log_{10}(\rho^2)$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from Fig 14b. The unfolded charged-particle $log_{10}(\rho^2)$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from Fig 14b. The unfolded charged-particle $log_{10}(\rho^2)$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from FigAux 4a. The unfolded all-particle $log_{10}(\rho^2)$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from FigAux 4a. The unfolded all-particle $log_{10}(\rho^2)$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from FigAux 4b. The unfolded charged-particle $log_{10}(\rho^2)$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from FigAux 4b. The unfolded charged-particle $log_{10}(\rho^2)$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from FigAux 5a. The unfolded $log_{10}(\rho^2)$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from FigAux 5a. The unfolded $log_{10}(\rho^2)$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from FigAux 5b. The unfolded charged-particle $log_{10}(\rho^2)$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from FigAux 5b. The unfolded charged-particle $log_{10}(\rho^2)$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from Fig 14c. The unfolded all-particle $z_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from Fig 14c. The unfolded all-particle $z_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from Fig 14d. The unfolded all-particle $z_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from Fig 14d. The unfolded all-particle $z_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 4c. The unfolded all-particle $z_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 4c. The unfolded all-particle $z_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 4d. The unfolded all-particle $z_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 4d. The unfolded all-particle $z_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 5c. The unfolded all-particle $z_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 5c. The unfolded all-particle $z_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 5d. The unfolded all-particle $z_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 5d. The unfolded all-particle $z_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from Fig 14e. The unfolded all-particle $R_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from Fig 14e. The unfolded all-particle $R_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from Fig 14f. The unfolded all-particle $R_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from Fig 14f. The unfolded all-particle $R_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 4e. The unfolded all-particle $R_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 4e. The unfolded all-particle $R_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 4f. The unfolded all-particle $R_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 4f. The unfolded all-particle $R_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 5e. The unfolded all-particle $R_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 5e. The unfolded all-particle $R_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 5f. The unfolded all-particle $R_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 5f. The unfolded all-particle $R_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from Fig 36-40a. The unfolded all-particle $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$. Each set of 10 bins corresponds to one $p_T$ bin in (300, 400, 600, 800, 1000, infinity) and 10 evenly spaced bins in $log_{10}(\rho^2)$ from -4.5 to -0.5.
Data from Fig 36-40a. The unfolded all-particle $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$. Each set of 10 bins corresponds to one $p_T$ bin in (300, 400, 600, 800, 1000, infinity) and 10 evenly spaced bins in $log_{10}(\rho^2)$ from -4.5 to -0.5.
Data from Fig 81-85a. The unfolded charged-particle $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $log_{10}(\rho^2)$ from -4.5 to -0.5.
Data from Fig 81-85a. The unfolded charged-particle $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $log_{10}(\rho^2)$ from -4.5 to -0.5.
Data from Fig 36-40b. The unfolded all-particle $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $log_{10}(\rho^2)$ from -4.5 to -0.5.
Data from Fig 36-40b. The unfolded all-particle $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $log_{10}(\rho^2)$ from -4.5 to -0.5.
Data from Fig 81-85b. The unfolded charged-particle $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $log_{10}(\rho^2)$ from -4.5 to -0.5.
Data from Fig 81-85b. The unfolded charged-particle $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $log_{10}(\rho^2)$ from -4.5 to -0.5.
Data from Fig 36-40c. The unfolded $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $log_{10}(\rho^2)$ from -4.5 to -0.5.
Data from Fig 36-40c. The unfolded $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $log_{10}(\rho^2)$ from -4.5 to -0.5.
Data from Fig 81-85c. The unfolded charged-particle $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $log_{10}(\rho^2)$ from -4.5 to -0.5.
Data from Fig 81-85c. The unfolded charged-particle $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $log_{10}(\rho^2)$ from -4.5 to -0.5.
Data from Fig 51-55a. The unfolded all-particle $z_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $z_g$ from 0.0 to 0.5.
Data from Fig 51-55a. The unfolded all-particle $z_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $z_g$ from 0.0 to 0.5.
Data from Fig 101-105a. The unfolded all-particle $z_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $z_g$ from 0.0 to 0.5.
Data from Fig 101-105a. The unfolded all-particle $z_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $z_g$ from 0.0 to 0.5.
Data from Fig 51-55b. The unfolded all-particle $z_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $z_g$ from 0.0 to 0.5.
Data from Fig 51-55b. The unfolded all-particle $z_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $z_g$ from 0.0 to 0.5.
Data from Fig 101-105b. The unfolded all-particle $z_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $z_g$ from 0.0 to 0.5.
Data from Fig 101-105b. The unfolded all-particle $z_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $z_g$ from 0.0 to 0.5.
Data from Fig 51-55c. The unfolded all-particle $z_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $z_g$ from 0.0 to 0.5.
Data from Fig 51-55c. The unfolded all-particle $z_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $z_g$ from 0.0 to 0.5.
Data from Fig 101-105c. The unfolded all-particle $z_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $z_g$ from 0.0 to 0.5.
Data from Fig 101-105c. The unfolded all-particle $z_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $z_g$ from 0.0 to 0.5.
Data from Fig 66-70a. The unfolded all-particle $R_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 6 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 6 bins in $r_g$ (0.06310, 0.10000, 0.15849, 0.25119, 0.39811, 0.63096, 0.80000).
Data from Fig 66-70a. The unfolded all-particle $R_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 6 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 6 bins in $r_g$ (0.06310, 0.10000, 0.15849, 0.25119, 0.39811, 0.63096, 0.80000).
Data from Fig 106-110a. The unfolded all-particle $R_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 6 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 6 bins in $r_g$ (0.06310, 0.10000, 0.15849, 0.25119, 0.39811, 0.63096, 0.80000).
Data from Fig 106-110a. The unfolded all-particle $R_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 6 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 6 bins in $r_g$ (0.06310, 0.10000, 0.15849, 0.25119, 0.39811, 0.63096, 0.80000).
Data from Fig 66-70b. The unfolded all-particle $R_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 6 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 6 bins in $r_g$ (0.06310, 0.10000, 0.15849, 0.25119, 0.39811, 0.63096, 0.80000).
Data from Fig 66-70b. The unfolded all-particle $R_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 6 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 6 bins in $r_g$ (0.06310, 0.10000, 0.15849, 0.25119, 0.39811, 0.63096, 0.80000).
Data from Fig 106-110b. The unfolded all-particle $R_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 6 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 6 bins in $r_g$ (0.06310, 0.10000, 0.15849, 0.25119, 0.39811, 0.63096, 0.80000).
Data from Fig 106-110b. The unfolded all-particle $R_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 6 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 6 bins in $r_g$ (0.06310, 0.10000, 0.15849, 0.25119, 0.39811, 0.63096, 0.80000).
Data from Fig 66-70c. The unfolded all-particle $R_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 6 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 6 bins in $r_g$ (0.06310, 0.10000, 0.15849, 0.25119, 0.39811, 0.63096, 0.80000).
Data from Fig 66-70c. The unfolded all-particle $R_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 6 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 6 bins in $r_g$ (0.06310, 0.10000, 0.15849, 0.25119, 0.39811, 0.63096, 0.80000).
Data from Fig 106-110c. The unfolded all-particle $R_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 6 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 6 bins in $r_g$ (0.06310, 0.10000, 0.15849, 0.25119, 0.39811, 0.63096, 0.80000).
Data from Fig 106-110c. The unfolded all-particle $R_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 6 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 6 bins in $r_g$ (0.06310, 0.10000, 0.15849, 0.25119, 0.39811, 0.63096, 0.80000).
Data from Fig 26-30a. The unfolded all-particle $log_{10}(\rho^2)$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $log_{10}(\rho^2)$ from -4.5 to -0.5.
Data from Fig 26-30a. The unfolded all-particle $log_{10}(\rho^2)$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $log_{10}(\rho^2)$ from -4.5 to -0.5.
Data from Fig 71-75a. The unfolded charged-particle $log_{10}(\rho^2)$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $log_{10}(\rho^2)$ from -4.5 to -0.5.
Data from Fig 71-75a. The unfolded charged-particle $log_{10}(\rho^2)$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $log_{10}(\rho^2)$ from -4.5 to -0.5.
Data from Fig 26-30b. The unfolded all-particle $log_{10}(\rho^2)$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $log_{10}(\rho^2)$ from -4.5 to -0.5.
Data from Fig 26-30b. The unfolded all-particle $log_{10}(\rho^2)$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $log_{10}(\rho^2)$ from -4.5 to -0.5.
Data from Fig 71-75b. The unfolded charged-particle $log_{10}(\rho^2)$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $log_{10}(\rho^2)$ from -4.5 to -0.5.
Data from Fig 71-75b. The unfolded charged-particle $log_{10}(\rho^2)$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $log_{10}(\rho^2)$ from -4.5 to -0.5.
Data from Fig 26-30c. The unfolded $log_{10}(\rho^2)$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $log_{10}(\rho^2)$ from -4.5 to -0.5.
Data from Fig 26-30c. The unfolded $log_{10}(\rho^2)$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $log_{10}(\rho^2)$ from -4.5 to -0.5.
Data from Fig 71-75c. The unfolded charged-particle $log_{10}(\rho^2)$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $log_{10}(\rho^2)$ from -4.5 to -0.5.
Data from Fig 71-75c. The unfolded charged-particle $log_{10}(\rho^2)$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $log_{10}(\rho^2)$ from -4.5 to -0.5.
Data from Fig 41-45a. The unfolded all-particle $z_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $z_g$ from 0.0 to 0.5.
Data from Fig 41-45a. The unfolded all-particle $z_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $z_g$ from 0.0 to 0.5.
Data from Fig 86-90a. The unfolded all-particle $z_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $z_g$ from 0.0 to 0.5.
Data from Fig 86-90a. The unfolded all-particle $z_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $z_g$ from 0.0 to 0.5.
Data from Fig 41-45b. The unfolded all-particle $z_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $z_g$ from 0.0 to 0.5.
Data from Fig 41-45b. The unfolded all-particle $z_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $z_g$ from 0.0 to 0.5.
Data from Fig 86-90b. The unfolded all-particle $z_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $z_g$ from 0.0 to 0.5.
Data from Fig 86-90b. The unfolded all-particle $z_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $z_g$ from 0.0 to 0.5.
Data from Fig 41-45c. The unfolded all-particle $z_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $z_g$ from 0.0 to 0.5.
Data from Fig 41-45c. The unfolded all-particle $z_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $z_g$ from 0.0 to 0.5.
Data from Fig 86-90c. The unfolded all-particle $z_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $z_g$ from 0.0 to 0.5.
Data from Fig 86-90c. The unfolded all-particle $z_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $z_g$ from 0.0 to 0.5.
Data from Fig 56-60a. The unfolded all-particle $R_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 6 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 6 bins in $r_g$ (0.06310, 0.10000, 0.15849, 0.25119, 0.39811, 0.63096, 0.80000).
Data from Fig 56-60a. The unfolded all-particle $R_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 6 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 6 bins in $r_g$ (0.06310, 0.10000, 0.15849, 0.25119, 0.39811, 0.63096, 0.80000).
Data from Fig 101-105a. The unfolded all-particle $R_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 6 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 6 bins in $r_g$ (0.06310, 0.10000, 0.15849, 0.25119, 0.39811, 0.63096, 0.80000).
Data from Fig 101-105a. The unfolded all-particle $R_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 6 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 6 bins in $r_g$ (0.06310, 0.10000, 0.15849, 0.25119, 0.39811, 0.63096, 0.80000).
Data from Fig 56-60b. The unfolded all-particle $R_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 6 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 6 bins in $r_g$ (0.06310, 0.10000, 0.15849, 0.25119, 0.39811, 0.63096, 0.80000).
Data from Fig 56-60b. The unfolded all-particle $R_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 6 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 6 bins in $r_g$ (0.06310, 0.10000, 0.15849, 0.25119, 0.39811, 0.63096, 0.80000).
Data from Fig 101-105b. The unfolded all-particle $R_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 6 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 6 bins in $r_g$ (0.06310, 0.10000, 0.15849, 0.25119, 0.39811, 0.63096, 0.80000).
Data from Fig 101-105b. The unfolded all-particle $R_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 6 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 6 bins in $r_g$ (0.06310, 0.10000, 0.15849, 0.25119, 0.39811, 0.63096, 0.80000).
Data from Fig 56-60c. The unfolded all-particle $R_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 6 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 6 bins in $r_g$ (0.06310, 0.10000, 0.15849, 0.25119, 0.39811, 0.63096, 0.80000).
Data from Fig 56-60c. The unfolded all-particle $R_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 6 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 6 bins in $r_g$ (0.06310, 0.10000, 0.15849, 0.25119, 0.39811, 0.63096, 0.80000).
Data from Fig 101-105c. The unfolded all-particle $R_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 6 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 6 bins in $r_g$ (0.06310, 0.10000, 0.15849, 0.25119, 0.39811, 0.63096, 0.80000).
Data from Fig 101-105c. The unfolded all-particle $R_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 6 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 6 bins in $r_g$ (0.06310, 0.10000, 0.15849, 0.25119, 0.39811, 0.63096, 0.80000).
Data from Fig 31-35a. The unfolded all-particle $log_{10}(\rho^2)$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $log_{10}(\rho^2)$ from -4.5 to -0.5.
Data from Fig 31-35a. The unfolded all-particle $log_{10}(\rho^2)$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $log_{10}(\rho^2)$ from -4.5 to -0.5.
Data from Fig 76-80a. The unfolded charged-particle $log_{10}(\rho^2)$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $log_{10}(\rho^2)$ from -4.5 to -0.5.
Data from Fig 76-80a. The unfolded charged-particle $log_{10}(\rho^2)$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $log_{10}(\rho^2)$ from -4.5 to -0.5.
Data from Fig 31-35b. The unfolded all-particle $log_{10}(\rho^2)$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $log_{10}(\rho^2)$ from -4.5 to -0.5.
Data from Fig 31-35b. The unfolded all-particle $log_{10}(\rho^2)$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $log_{10}(\rho^2)$ from -4.5 to -0.5.
Data from Fig 76-80b. The unfolded charged-particle $log_{10}(\rho^2)$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $log_{10}(\rho^2)$ from -4.5 to -0.5.
Data from Fig 76-80b. The unfolded charged-particle $log_{10}(\rho^2)$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $log_{10}(\rho^2)$ from -4.5 to -0.5.
Data from Fig 31-35c. The unfolded $log_{10}(\rho^2)$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $log_{10}(\rho^2)$ from -4.5 to -0.5.
Data from Fig 31-35c. The unfolded $log_{10}(\rho^2)$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $log_{10}(\rho^2)$ from -4.5 to -0.5.
Data from Fig 76-80c. The unfolded charged-particle $log_{10}(\rho^2)$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $log_{10}(\rho^2)$ from -4.5 to -0.5.
Data from Fig 76-80c. The unfolded charged-particle $log_{10}(\rho^2)$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $log_{10}(\rho^2)$ from -4.5 to -0.5.
Data from Fig 46-50a. The unfolded all-particle $z_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $z_g$ from 0.0 to 0.5.
Data from Fig 46-50a. The unfolded all-particle $z_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $z_g$ from 0.0 to 0.5.
Data from Fig 91-95a. The unfolded all-particle $z_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $z_g$ from 0.0 to 0.5.
Data from Fig 91-95a. The unfolded all-particle $z_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $z_g$ from 0.0 to 0.5.
Data from Fig 46-50b. The unfolded all-particle $z_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $z_g$ from 0.0 to 0.5.
Data from Fig 46-50b. The unfolded all-particle $z_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $z_g$ from 0.0 to 0.5.
Data from Fig 91-95b. The unfolded all-particle $z_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $z_g$ from 0.0 to 0.5.
Data from Fig 91-95b. The unfolded all-particle $z_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $z_g$ from 0.0 to 0.5.
Data from Fig 46-50c. The unfolded all-particle $z_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $z_g$ from 0.0 to 0.5.
Data from Fig 46-50c. The unfolded all-particle $z_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $z_g$ from 0.0 to 0.5.
Data from Fig 91-95c. The unfolded all-particle $z_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $z_g$ from 0.0 to 0.5.
Data from Fig 91-95c. The unfolded all-particle $z_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $z_g$ from 0.0 to 0.5.
Data from Fig 61-65a. The unfolded all-particle $R_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 6 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 6 bins in $r_g$ (0.06310, 0.10000, 0.15849, 0.25119, 0.39811, 0.63096, 0.80000).
Data from Fig 61-65a. The unfolded all-particle $R_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 6 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 6 bins in $r_g$ (0.06310, 0.10000, 0.15849, 0.25119, 0.39811, 0.63096, 0.80000).
Data from Fig 106-110a. The unfolded all-particle $R_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 6 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 6 bins in $r_g$ (0.06310, 0.10000, 0.15849, 0.25119, 0.39811, 0.63096, 0.80000).
Data from Fig 106-110a. The unfolded all-particle $R_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 6 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 6 bins in $r_g$ (0.06310, 0.10000, 0.15849, 0.25119, 0.39811, 0.63096, 0.80000).
Data from Fig 61-65b. The unfolded all-particle $R_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 6 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 6 bins in $r_g$ (0.06310, 0.10000, 0.15849, 0.25119, 0.39811, 0.63096, 0.80000).
Data from Fig 61-65b. The unfolded all-particle $R_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 6 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 6 bins in $r_g$ (0.06310, 0.10000, 0.15849, 0.25119, 0.39811, 0.63096, 0.80000).
Data from Fig 106-110b. The unfolded all-particle $R_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 6 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 6 bins in $r_g$ (0.06310, 0.10000, 0.15849, 0.25119, 0.39811, 0.63096, 0.80000).
Data from Fig 106-110b. The unfolded all-particle $R_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 6 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 6 bins in $r_g$ (0.06310, 0.10000, 0.15849, 0.25119, 0.39811, 0.63096, 0.80000).
Data from Fig 61-65c. The unfolded all-particle $R_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 6 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 6 bins in $r_g$ (0.06310, 0.10000, 0.15849, 0.25119, 0.39811, 0.63096, 0.80000).
Data from Fig 61-65c. The unfolded all-particle $R_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 6 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 6 bins in $r_g$ (0.06310, 0.10000, 0.15849, 0.25119, 0.39811, 0.63096, 0.80000).
Data from Fig 106-110c. The unfolded all-particle $R_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 6 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 6 bins in $r_g$ (0.06310, 0.10000, 0.15849, 0.25119, 0.39811, 0.63096, 0.80000).
Data from Fig 106-110c. The unfolded all-particle $R_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 6 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 6 bins in $r_g$ (0.06310, 0.10000, 0.15849, 0.25119, 0.39811, 0.63096, 0.80000).
Data from FigAux 6a. The extracted quark-distribution from the unfolded all-particle $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with 600 < $p_T$ < 800 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from FigAux 6a. The extracted quark-distribution from the unfolded all-particle $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with 600 < $p_T$ < 800 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from Fig 15a. Theextracted quark-distribution from the unfolded charged-particle $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with 600 < $p_T$ < 800 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from Fig 15a. Theextracted quark-distribution from the unfolded charged-particle $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with 600 < $p_T$ < 800 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from FigAux 6b. The extracted quark-distribution from the unfolded all-particle $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with 600 < $p_T$ < 800 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from FigAux 6b. The extracted quark-distribution from the unfolded all-particle $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with 600 < $p_T$ < 800 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from Fig 15b. The extracted quark-distribution from the unfolded charged-particle $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with 600 < $p_T$ < 800 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from Fig 15b. The extracted quark-distribution from the unfolded charged-particle $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with 600 < $p_T$ < 800 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from FigAux 6c. The extracted quark-distribution from the unfolded all-particle $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with 600 < $p_T$ < 800 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from FigAux 6c. The extracted quark-distribution from the unfolded all-particle $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with 600 < $p_T$ < 800 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from Fig 15c. The extracted quark-distribution from the unfolded charged-particle $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with 600 < $p_T$ < 800 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from Fig 15c. The extracted quark-distribution from the unfolded charged-particle $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with 600 < $p_T$ < 800 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from FigAux 7a. The extracted quark-distribution from the unfolded all-particle $z_g$ distribution for anti-kt R=0.8 jets with 600 < $p_T$ < 800 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 7a. The extracted quark-distribution from the unfolded all-particle $z_g$ distribution for anti-kt R=0.8 jets with 600 < $p_T$ < 800 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from Fig 16a. The extracted quark-distribution from the unfolded charged-particle $z_g$ distribution for anti-kt R=0.8 jets with 600 < $p_T$ < 800 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from Fig 16a. The extracted quark-distribution from the unfolded charged-particle $z_g$ distribution for anti-kt R=0.8 jets with 600 < $p_T$ < 800 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 7b. The extracted quark-distribution from the unfolded all-particle $z_g$ distribution for anti-kt R=0.8 jets with 600 < $p_T$ < 800 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 7b. The extracted quark-distribution from the unfolded all-particle $z_g$ distribution for anti-kt R=0.8 jets with 600 < $p_T$ < 800 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from Fig 16b. The extracted quark-distribution from the unfolded charged-particle $z_g$ distribution for anti-kt R=0.8 jets with 600 < $p_T$ < 800 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from Fig 16b. The extracted quark-distribution from the unfolded charged-particle $z_g$ distribution for anti-kt R=0.8 jets with 600 < $p_T$ < 800 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 7c. The extracted quark-distribution from the unfolded all-particle $z_g$ distribution for anti-kt R=0.8 jets with 600 < $p_T$ < 800 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 7c. The extracted quark-distribution from the unfolded all-particle $z_g$ distribution for anti-kt R=0.8 jets with 600 < $p_T$ < 800 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from Fig 16c. The extracted quark-distribution from the unfolded charged-particle $z_g$ distribution for anti-kt R=0.8 jets with 600 < $p_T$ < 800 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from Fig 16c. The extracted quark-distribution from the unfolded charged-particle $z_g$ distribution for anti-kt R=0.8 jets with 600 < $p_T$ < 800 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 8a. The extracted quark-distribution from the unfolded all-particle $R_g$ distribution for anti-kt R=0.8 jets with 600 < $p_T$ < 800 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 8a. The extracted quark-distribution from the unfolded all-particle $R_g$ distribution for anti-kt R=0.8 jets with 600 < $p_T$ < 800 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from Fig 17a. The extracted quark-distribution from the unfolded charged-particle $R_g$ distribution for anti-kt R=0.8 jets with 600 < $p_T$ < 800 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from Fig 17a. The extracted quark-distribution from the unfolded charged-particle $R_g$ distribution for anti-kt R=0.8 jets with 600 < $p_T$ < 800 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 8b. The extracted quark-distribution from the unfolded all-particle $R_g$ distribution for anti-kt R=0.8 jets with 600 < $p_T$ < 800 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 8b. The extracted quark-distribution from the unfolded all-particle $R_g$ distribution for anti-kt R=0.8 jets with 600 < $p_T$ < 800 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from Fig 17b. The extracted quark-distribution from the unfolded charged-particle $R_g$ distribution for anti-kt R=0.8 jets with 600 < $p_T$ < 800 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from Fig 17b. The extracted quark-distribution from the unfolded charged-particle $R_g$ distribution for anti-kt R=0.8 jets with 600 < $p_T$ < 800 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 8c. The extracted quark-distribution from the unfolded all-particle $R_g$ distribution for anti-kt R=0.8 jets with 600 < $p_T$ < 800 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 8c. The extracted quark-distribution from the unfolded all-particle $R_g$ distribution for anti-kt R=0.8 jets with 600 < $p_T$ < 800 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from Fig 17c. The extracted quark-distribution from the unfolded charged-particle $R_g$ distribution for anti-kt R=0.8 jets with 600 < $p_T$ < 800 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from Fig 17c. The extracted quark-distribution from the unfolded charged-particle $R_g$ distribution for anti-kt R=0.8 jets with 600 < $p_T$ < 800 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 6a. The extracted gluon-distribution from the unfolded all-particle $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with 600 < $p_T$ < 800 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from FigAux 6a. The extracted gluon-distribution from the unfolded all-particle $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with 600 < $p_T$ < 800 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from Fig 15a. Theextracted gluon-distribution from the unfolded charged-particle $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with 600 < $p_T$ < 800 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from Fig 15a. Theextracted gluon-distribution from the unfolded charged-particle $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with 600 < $p_T$ < 800 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from FigAux 6b. The extracted gluon-distribution from the unfolded all-particle $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with 600 < $p_T$ < 800 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from FigAux 6b. The extracted gluon-distribution from the unfolded all-particle $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with 600 < $p_T$ < 800 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from Fig 15b. The extracted gluon-distribution from the unfolded charged-particle $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with 600 < $p_T$ < 800 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from Fig 15b. The extracted gluon-distribution from the unfolded charged-particle $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with 600 < $p_T$ < 800 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from FigAux 6c. The extracted gluon-distribution from the unfolded all-particle $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with 600 < $p_T$ < 800 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from FigAux 6c. The extracted gluon-distribution from the unfolded all-particle $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with 600 < $p_T$ < 800 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from Fig 15c. The extracted gluon-distribution from the unfolded charged-particle $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with 600 < $p_T$ < 800 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from Fig 15c. The extracted gluon-distribution from the unfolded charged-particle $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with 600 < $p_T$ < 800 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from FigAux 7a. The extracted gluon-distribution from the unfolded all-particle $z_g$ distribution for anti-kt R=0.8 jets with 600 < $p_T$ < 800 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 7a. The extracted gluon-distribution from the unfolded all-particle $z_g$ distribution for anti-kt R=0.8 jets with 600 < $p_T$ < 800 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from Fig 16a. The extracted gluon-distribution from the unfolded charged-particle $z_g$ distribution for anti-kt R=0.8 jets with 600 < $p_T$ < 800 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from Fig 16a. The extracted gluon-distribution from the unfolded charged-particle $z_g$ distribution for anti-kt R=0.8 jets with 600 < $p_T$ < 800 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 7b. The extracted gluon-distribution from the unfolded all-particle $z_g$ distribution for anti-kt R=0.8 jets with 600 < $p_T$ < 800 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 7b. The extracted gluon-distribution from the unfolded all-particle $z_g$ distribution for anti-kt R=0.8 jets with 600 < $p_T$ < 800 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from Fig 16b. The extracted gluon-distribution from the unfolded charged-particle $z_g$ distribution for anti-kt R=0.8 jets with 600 < $p_T$ < 800 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from Fig 16b. The extracted gluon-distribution from the unfolded charged-particle $z_g$ distribution for anti-kt R=0.8 jets with 600 < $p_T$ < 800 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 7c. The extracted gluon-distribution from the unfolded all-particle $z_g$ distribution for anti-kt R=0.8 jets with 600 < $p_T$ < 800 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 7c. The extracted gluon-distribution from the unfolded all-particle $z_g$ distribution for anti-kt R=0.8 jets with 600 < $p_T$ < 800 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from Fig 16c. The extracted gluon-distribution from the unfolded charged-particle $z_g$ distribution for anti-kt R=0.8 jets with 600 < $p_T$ < 800 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from Fig 16c. The extracted gluon-distribution from the unfolded charged-particle $z_g$ distribution for anti-kt R=0.8 jets with 600 < $p_T$ < 800 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 8a. The extracted gluon-distribution from the unfolded all-particle $R_g$ distribution for anti-kt R=0.8 jets with 600 < $p_T$ < 800 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 8a. The extracted gluon-distribution from the unfolded all-particle $R_g$ distribution for anti-kt R=0.8 jets with 600 < $p_T$ < 800 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from Fig 17a. The extracted gluon-distribution from the unfolded charged-particle $R_g$ distribution for anti-kt R=0.8 jets with 600 < $p_T$ < 800 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from Fig 17a. The extracted gluon-distribution from the unfolded charged-particle $R_g$ distribution for anti-kt R=0.8 jets with 600 < $p_T$ < 800 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 8b. The extracted gluon-distribution from the unfolded all-particle $R_g$ distribution for anti-kt R=0.8 jets with 600 < $p_T$ < 800 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 8b. The extracted gluon-distribution from the unfolded all-particle $R_g$ distribution for anti-kt R=0.8 jets with 600 < $p_T$ < 800 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from Fig 17b. The extracted gluon-distribution from the unfolded charged-particle $R_g$ distribution for anti-kt R=0.8 jets with 600 < $p_T$ < 800 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from Fig 17b. The extracted gluon-distribution from the unfolded charged-particle $R_g$ distribution for anti-kt R=0.8 jets with 600 < $p_T$ < 800 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 8c. The extracted gluon-distribution from the unfolded all-particle $R_g$ distribution for anti-kt R=0.8 jets with 600 < $p_T$ < 800 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 8c. The extracted gluon-distribution from the unfolded all-particle $R_g$ distribution for anti-kt R=0.8 jets with 600 < $p_T$ < 800 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from Fig 17c. The extracted gluon-distribution from the unfolded charged-particle $R_g$ distribution for anti-kt R=0.8 jets with 600 < $p_T$ < 800 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from Fig 17c. The extracted gluon-distribution from the unfolded charged-particle $R_g$ distribution for anti-kt R=0.8 jets with 600 < $p_T$ < 800 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 99a. The full covariance matrices for the all-particle $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from FigAux 99a. The full covariance matrices for the all-particle $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from FigAux 100a. The full covariance matrices for the charged-particle $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from FigAux 100a. The full covariance matrices for the charged-particle $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from FigAux 99b. The full covariance matrices for the all-particle $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from FigAux 99b. The full covariance matrices for the all-particle $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from FigAux 100b. The full covariance matrices for the charged-particle $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from FigAux 100b. The full covariance matrices for the charged-particle $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from FigAux 99c. The full covariance matrices for the $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from FigAux 99c. The full covariance matrices for the $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from FigAux 100c. The full covariance matrices for the charged-particle $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from FigAux 100c. The full covariance matrices for the charged-particle $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from FigAux 101a. The full covariance matrices for the all-particle $z_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 101a. The full covariance matrices for the all-particle $z_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 102a. The full covariance matrices for the all-particle $z_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 102a. The full covariance matrices for the all-particle $z_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 101b. The full covariance matrices for the all-particle $z_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 101b. The full covariance matrices for the all-particle $z_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 102b. The full covariance matrices for the all-particle $z_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 102b. The full covariance matrices for the all-particle $z_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 101c. The full covariance matrices for the all-particle $z_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 101c. The full covariance matrices for the all-particle $z_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 102c. The full covariance matrices for the all-particle $z_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 102c. The full covariance matrices for the all-particle $z_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 103a. The full covariance matrices for the all-particle $R_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 103a. The full covariance matrices for the all-particle $R_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 104a. The full covariance matrices for the all-particle $R_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 104a. The full covariance matrices for the all-particle $R_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 103b. The full covariance matrices for the all-particle $R_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 103b. The full covariance matrices for the all-particle $R_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 104b. The full covariance matrices for the all-particle $R_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 104b. The full covariance matrices for the all-particle $R_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 103c. The full covariance matrices for the all-particle $R_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 103c. The full covariance matrices for the all-particle $R_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 104c. The full covariance matrices for the all-particle $R_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 104c. The full covariance matrices for the all-particle $R_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 105a. The full covariance matrices for the all-particle $log_{10}(\rho^2)$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from FigAux 105a. The full covariance matrices for the all-particle $log_{10}(\rho^2)$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from FigAux 106a. The full covariance matrices for the charged-particle $log_{10}(\rho^2)$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from FigAux 106a. The full covariance matrices for the charged-particle $log_{10}(\rho^2)$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from FigAux 105b. The full covariance matrices for the all-particle $log_{10}(\rho^2)$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from FigAux 105b. The full covariance matrices for the all-particle $log_{10}(\rho^2)$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from FigAux 106b. The full covariance matrices for the charged-particle $log_{10}(\rho^2)$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from FigAux 106b. The full covariance matrices for the charged-particle $log_{10}(\rho^2)$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from FigAux 105c. The full covariance matrices for the $log_{10}(\rho^2)$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from FigAux 105c. The full covariance matrices for the $log_{10}(\rho^2)$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from FigAux 106c. The full covariance matrices for the charged-particle $log_{10}(\rho^2)$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from FigAux 106c. The full covariance matrices for the charged-particle $log_{10}(\rho^2)$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from FigAux 107a. The full covariance matrices for the all-particle $z_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 107a. The full covariance matrices for the all-particle $z_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 108a. The full covariance matrices for the all-particle $z_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 108a. The full covariance matrices for the all-particle $z_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 107b. The full covariance matrices for the all-particle $z_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 107b. The full covariance matrices for the all-particle $z_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 108b. The full covariance matrices for the all-particle $z_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 108b. The full covariance matrices for the all-particle $z_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 107c. The full covariance matrices for the all-particle $z_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 107c. The full covariance matrices for the all-particle $z_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 108c. The full covariance matrices for the all-particle $z_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 108c. The full covariance matrices for the all-particle $z_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 109a. The full covariance matrices for the all-particle $R_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 109a. The full covariance matrices for the all-particle $R_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 110a. The full covariance matrices for the all-particle $R_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 110a. The full covariance matrices for the all-particle $R_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 109b. The full covariance matrices for the all-particle $R_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 109b. The full covariance matrices for the all-particle $R_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 110b. The full covariance matrices for the all-particle $R_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 110b. The full covariance matrices for the all-particle $R_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 109c. The full covariance matrices for the all-particle $R_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 109c. The full covariance matrices for the all-particle $R_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 110c. The full covariance matrices for the all-particle $R_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 110c. The full covariance matrices for the all-particle $R_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 111a. The full covariance matrices for the all-particle $log_{10}(\rho^2)$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from FigAux 111a. The full covariance matrices for the all-particle $log_{10}(\rho^2)$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from FigAux 112a. The full covariance matrices for the charged-particle $log_{10}(\rho^2)$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from FigAux 112a. The full covariance matrices for the charged-particle $log_{10}(\rho^2)$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from FigAux 111b. The full covariance matrices for the all-particle $log_{10}(\rho^2)$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from FigAux 111b. The full covariance matrices for the all-particle $log_{10}(\rho^2)$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from FigAux 112b. The full covariance matrices for the charged-particle $log_{10}(\rho^2)$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from FigAux 112b. The full covariance matrices for the charged-particle $log_{10}(\rho^2)$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from FigAux 111c. The full covariance matrices for the $log_{10}(\rho^2)$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from FigAux 111c. The full covariance matrices for the $log_{10}(\rho^2)$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from FigAux 112c. The full covariance matrices for the charged-particle $log_{10}(\rho^2)$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from FigAux 112c. The full covariance matrices for the charged-particle $log_{10}(\rho^2)$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from FigAux 113a. The full covariance matrices for the all-particle $z_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 113a. The full covariance matrices for the all-particle $z_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 114a. The full covariance matrices for the all-particle $z_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 114a. The full covariance matrices for the all-particle $z_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 113b. The full covariance matrices for the all-particle $z_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 113b. The full covariance matrices for the all-particle $z_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 114b. The full covariance matrices for the all-particle $z_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 114b. The full covariance matrices for the all-particle $z_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 113c. The full covariance matrices for the all-particle $z_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 113c. The full covariance matrices for the all-particle $z_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 114c. The full covariance matrices for the all-particle $z_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 114c. The full covariance matrices for the all-particle $z_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 115a. The full covariance matrices for the all-particle $R_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 115a. The full covariance matrices for the all-particle $R_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 116a. The full covariance matrices for the all-particle $R_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 116a. The full covariance matrices for the all-particle $R_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 115b. The full covariance matrices for the all-particle $R_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 115b. The full covariance matrices for the all-particle $R_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 116b. The full covariance matrices for the all-particle $R_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 116b. The full covariance matrices for the all-particle $R_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 115c. The full covariance matrices for the all-particle $R_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 115c. The full covariance matrices for the all-particle $R_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 116c. The full covariance matrices for the all-particle $R_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 116c. The full covariance matrices for the all-particle $R_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. The distributions are normalized to the integrated cross section, $\sigma$.
Data from FigAux 99d. The full covariance matrices for the all-particle $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $log_{10}(\rho^2)$ from -4.5 to -0.5.
Data from FigAux 99d. The full covariance matrices for the all-particle $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $log_{10}(\rho^2)$ from -4.5 to -0.5.
Data from FigAux 100d. The full covariance matrices for the charged-particle $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $log_{10}(\rho^2)$ from -4.5 to -0.5.
Data from FigAux 100d. The full covariance matrices for the charged-particle $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $log_{10}(\rho^2)$ from -4.5 to -0.5.
Data from FigAux 99e. The full covariance matrices for the all-particle $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $log_{10}(\rho^2)$ from -4.5 to -0.5.
Data from FigAux 99e. The full covariance matrices for the all-particle $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $log_{10}(\rho^2)$ from -4.5 to -0.5.
Data from FigAux 100e. The full covariance matrices for the charged-particle $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $log_{10}(\rho^2)$ from -4.5 to -0.5.
Data from FigAux 100e. The full covariance matrices for the charged-particle $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $log_{10}(\rho^2)$ from -4.5 to -0.5.
Data from FigAux 99f. The full covariance matrices for the $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $log_{10}(\rho^2)$ from -4.5 to -0.5.
Data from FigAux 99f. The full covariance matrices for the $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $log_{10}(\rho^2)$ from -4.5 to -0.5.
Data from FigAux 100f. The full covariance matrices for the charged-particle $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $log_{10}(\rho^2)$ from -4.5 to -0.5.
Data from FigAux 100f. The full covariance matrices for the charged-particle $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $log_{10}(\rho^2)$ from -4.5 to -0.5.
Data from FigAux 101d. The full covariance matrices for the all-particle $z_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $z_g$ from 0.0 to 0.5.
Data from FigAux 101d. The full covariance matrices for the all-particle $z_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $z_g$ from 0.0 to 0.5.
Data from FigAux 102d. The full covariance matrices for the all-particle $z_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $z_g$ from 0.0 to 0.5.
Data from FigAux 102d. The full covariance matrices for the all-particle $z_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $z_g$ from 0.0 to 0.5.
Data from FigAux 101e. The full covariance matrices for the all-particle $z_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $z_g$ from 0.0 to 0.5.
Data from FigAux 101e. The full covariance matrices for the all-particle $z_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $z_g$ from 0.0 to 0.5.
Data from FigAux 102e. The full covariance matrices for the all-particle $z_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $z_g$ from 0.0 to 0.5.
Data from FigAux 102e. The full covariance matrices for the all-particle $z_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $z_g$ from 0.0 to 0.5.
Data from FigAux 101f. The full covariance matrices for the all-particle $z_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $z_g$ from 0.0 to 0.5.
Data from FigAux 101f. The full covariance matrices for the all-particle $z_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $z_g$ from 0.0 to 0.5.
Data from FigAux 102f. The full covariance matrices for the all-particle $z_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $z_g$ from 0.0 to 0.5.
Data from FigAux 102f. The full covariance matrices for the all-particle $z_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $z_g$ from 0.0 to 0.5.
Data from FigAux 103d. The full covariance matrices for the all-particle $R_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 6 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 6 bins in $r_g$ (0.06310, 0.10000, 0.15849, 0.25119, 0.39811, 0.63096, 0.80000).
Data from FigAux 103d. The full covariance matrices for the all-particle $R_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 6 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 6 bins in $r_g$ (0.06310, 0.10000, 0.15849, 0.25119, 0.39811, 0.63096, 0.80000).
Data from FigAux 104d. The full covariance matrices for the all-particle $R_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 6 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 6 bins in $r_g$ (0.06310, 0.10000, 0.15849, 0.25119, 0.39811, 0.63096, 0.80000).
Data from FigAux 104d. The full covariance matrices for the all-particle $R_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 6 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 6 bins in $r_g$ (0.06310, 0.10000, 0.15849, 0.25119, 0.39811, 0.63096, 0.80000).
Data from FigAux 103e. The full covariance matrices for the all-particle $R_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 6 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 6 bins in $r_g$ (0.06310, 0.10000, 0.15849, 0.25119, 0.39811, 0.63096, 0.80000).
Data from FigAux 103e. The full covariance matrices for the all-particle $R_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 6 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 6 bins in $r_g$ (0.06310, 0.10000, 0.15849, 0.25119, 0.39811, 0.63096, 0.80000).
Data from FigAux 104e. The full covariance matrices for the all-particle $R_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 6 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 6 bins in $r_g$ (0.06310, 0.10000, 0.15849, 0.25119, 0.39811, 0.63096, 0.80000).
Data from FigAux 104e. The full covariance matrices for the all-particle $R_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 6 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 6 bins in $r_g$ (0.06310, 0.10000, 0.15849, 0.25119, 0.39811, 0.63096, 0.80000).
Data from FigAux 103f. The full covariance matrices for the all-particle $R_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 6 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 6 bins in $r_g$ (0.06310, 0.10000, 0.15849, 0.25119, 0.39811, 0.63096, 0.80000).
Data from FigAux 103f. The full covariance matrices for the all-particle $R_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 6 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 6 bins in $r_g$ (0.06310, 0.10000, 0.15849, 0.25119, 0.39811, 0.63096, 0.80000).
Data from FigAux 104f. The full covariance matrices for the all-particle $R_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 6 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 6 bins in $r_g$ (0.06310, 0.10000, 0.15849, 0.25119, 0.39811, 0.63096, 0.80000).
Data from FigAux 104f. The full covariance matrices for the all-particle $R_g$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 6 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 6 bins in $r_g$ (0.06310, 0.10000, 0.15849, 0.25119, 0.39811, 0.63096, 0.80000).
Data from FigAux 105d. The full covariance matrices for the all-particle $log_{10}(\rho^2)$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $log_{10}(\rho^2)$ from -4.5 to -0.5.
Data from FigAux 105d. The full covariance matrices for the all-particle $log_{10}(\rho^2)$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $log_{10}(\rho^2)$ from -4.5 to -0.5.
Data from FigAux 106d. The full covariance matrices for the charged-particle $log_{10}(\rho^2)$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $log_{10}(\rho^2)$ from -4.5 to -0.5.
Data from FigAux 106d. The full covariance matrices for the charged-particle $log_{10}(\rho^2)$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $log_{10}(\rho^2)$ from -4.5 to -0.5.
Data from FigAux 105e. The full covariance matrices for the all-particle $log_{10}(\rho^2)$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $log_{10}(\rho^2)$ from -4.5 to -0.5.
Data from FigAux 105e. The full covariance matrices for the all-particle $log_{10}(\rho^2)$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $log_{10}(\rho^2)$ from -4.5 to -0.5.
Data from FigAux 106e. The full covariance matrices for the charged-particle $log_{10}(\rho^2)$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $log_{10}(\rho^2)$ from -4.5 to -0.5.
Data from FigAux 106e. The full covariance matrices for the charged-particle $log_{10}(\rho^2)$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $log_{10}(\rho^2)$ from -4.5 to -0.5.
Data from FigAux 105f. The full covariance matrices for the $log_{10}(\rho^2)$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $log_{10}(\rho^2)$ from -4.5 to -0.5.
Data from FigAux 105f. The full covariance matrices for the $log_{10}(\rho^2)$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $log_{10}(\rho^2)$ from -4.5 to -0.5.
Data from FigAux 106f. The full covariance matrices for the charged-particle $log_{10}(\rho^2)$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $log_{10}(\rho^2)$ from -4.5 to -0.5.
Data from FigAux 106f. The full covariance matrices for the charged-particle $log_{10}(\rho^2)$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $log_{10}(\rho^2)$ from -4.5 to -0.5.
Data from FigAux 107d. The full covariance matrices for the all-particle $z_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $z_g$ from 0.0 to 0.5.
Data from FigAux 107d. The full covariance matrices for the all-particle $z_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $z_g$ from 0.0 to 0.5.
Data from FigAux 108d. The full covariance matrices for the all-particle $z_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $z_g$ from 0.0 to 0.5.
Data from FigAux 108d. The full covariance matrices for the all-particle $z_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $z_g$ from 0.0 to 0.5.
Data from FigAux 107e. The full covariance matrices for the all-particle $z_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $z_g$ from 0.0 to 0.5.
Data from FigAux 107e. The full covariance matrices for the all-particle $z_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $z_g$ from 0.0 to 0.5.
Data from FigAux 108e. The full covariance matrices for the all-particle $z_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $z_g$ from 0.0 to 0.5.
Data from FigAux 108e. The full covariance matrices for the all-particle $z_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $z_g$ from 0.0 to 0.5.
Data from FigAux 107f. The full covariance matrices for the all-particle $z_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $z_g$ from 0.0 to 0.5.
Data from FigAux 107f. The full covariance matrices for the all-particle $z_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $z_g$ from 0.0 to 0.5.
Data from FigAux 108f. The full covariance matrices for the all-particle $z_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $z_g$ from 0.0 to 0.5.
Data from FigAux 108f. The full covariance matrices for the all-particle $z_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $z_g$ from 0.0 to 0.5.
Data from FigAux 109d. The full covariance matrices for the all-particle $R_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 6 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 6 bins in $r_g$ (0.06310, 0.10000, 0.15849, 0.25119, 0.39811, 0.63096, 0.80000).
Data from FigAux 109d. The full covariance matrices for the all-particle $R_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 6 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 6 bins in $r_g$ (0.06310, 0.10000, 0.15849, 0.25119, 0.39811, 0.63096, 0.80000).
Data from FigAux 110d. The full covariance matrices for the all-particle $R_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 6 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 6 bins in $r_g$ (0.06310, 0.10000, 0.15849, 0.25119, 0.39811, 0.63096, 0.80000).
Data from FigAux 110d. The full covariance matrices for the all-particle $R_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 6 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 6 bins in $r_g$ (0.06310, 0.10000, 0.15849, 0.25119, 0.39811, 0.63096, 0.80000).
Data from FigAux 109e. The full covariance matrices for the all-particle $R_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 6 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 6 bins in $r_g$ (0.06310, 0.10000, 0.15849, 0.25119, 0.39811, 0.63096, 0.80000).
Data from FigAux 109e. The full covariance matrices for the all-particle $R_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 6 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 6 bins in $r_g$ (0.06310, 0.10000, 0.15849, 0.25119, 0.39811, 0.63096, 0.80000).
Data from FigAux 110e. The full covariance matrices for the all-particle $R_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 6 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 6 bins in $r_g$ (0.06310, 0.10000, 0.15849, 0.25119, 0.39811, 0.63096, 0.80000).
Data from FigAux 110e. The full covariance matrices for the all-particle $R_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 6 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 6 bins in $r_g$ (0.06310, 0.10000, 0.15849, 0.25119, 0.39811, 0.63096, 0.80000).
Data from FigAux 109f. The full covariance matrices for the all-particle $R_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 6 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 6 bins in $r_g$ (0.06310, 0.10000, 0.15849, 0.25119, 0.39811, 0.63096, 0.80000).
Data from FigAux 109f. The full covariance matrices for the all-particle $R_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 6 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 6 bins in $r_g$ (0.06310, 0.10000, 0.15849, 0.25119, 0.39811, 0.63096, 0.80000).
Data from FigAux 110f. The full covariance matrices for the all-particle $R_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 6 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 6 bins in $r_g$ (0.06310, 0.10000, 0.15849, 0.25119, 0.39811, 0.63096, 0.80000).
Data from FigAux 110f. The full covariance matrices for the all-particle $R_g$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 6 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 6 bins in $r_g$ (0.06310, 0.10000, 0.15849, 0.25119, 0.39811, 0.63096, 0.80000).
Data from FigAux 111d. The full covariance matrices for the all-particle $log_{10}(\rho^2)$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from FigAux 111d. The full covariance matrices for the all-particle $log_{10}(\rho^2)$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from FigAux 112d. The full covariance matrices for the charged-particle $log_{10}(\rho^2)$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from FigAux 112d. The full covariance matrices for the charged-particle $log_{10}(\rho^2)$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from FigAux 111e. The full covariance matrices for the all-particle $log_{10}(\rho^2)$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from FigAux 111e. The full covariance matrices for the all-particle $log_{10}(\rho^2)$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from FigAux 112e. The full covariance matrices for the charged-particle $log_{10}(\rho^2)$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $log_{10}(\rho^2)$ from -4.5 to -0.5.
Data from FigAux 112e. The full covariance matrices for the charged-particle $log_{10}(\rho^2)$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $log_{10}(\rho^2)$ from -4.5 to -0.5.
Data from FigAux 111f. The full covariance matrices for the $log_{10}(\rho^2)$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $log_{10}(\rho^2)$ from -4.5 to -0.5.
Data from FigAux 111f. The full covariance matrices for the $log_{10}(\rho^2)$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $log_{10}(\rho^2)$ from -4.5 to -0.5.
Data from FigAux 112f. The full covariance matrices for the charged-particle $log_{10}(\rho^2)$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $log_{10}(\rho^2)$ from -4.5 to -0.5.
Data from FigAux 112f. The full covariance matrices for the charged-particle $log_{10}(\rho^2)$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $log_{10}(\rho^2)$ from -4.5 to -0.5.
Data from FigAux 113d. The full covariance matrices for the all-particle $z_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $z_g$ from 0.0 to 0.5.
Data from FigAux 113d. The full covariance matrices for the all-particle $z_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $z_g$ from 0.0 to 0.5.
Data from FigAux 114d. The full covariance matrices for the all-particle $z_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $z_g$ from 0.0 to 0.5.
Data from FigAux 114d. The full covariance matrices for the all-particle $z_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $z_g$ from 0.0 to 0.5.
Data from FigAux 113e. The full covariance matrices for the all-particle $z_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $z_g$ from 0.0 to 0.5.
Data from FigAux 113e. The full covariance matrices for the all-particle $z_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $z_g$ from 0.0 to 0.5.
Data from FigAux 114e. The full covariance matrices for the all-particle $z_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $z_g$ from 0.0 to 0.5.
Data from FigAux 114e. The full covariance matrices for the all-particle $z_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $z_g$ from 0.0 to 0.5.
Data from FigAux 113f. The full covariance matrices for the all-particle $z_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $z_g$ from 0.0 to 0.5.
Data from FigAux 113f. The full covariance matrices for the all-particle $z_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $z_g$ from 0.0 to 0.5.
Data from FigAux 114f. The full covariance matrices for the all-particle $z_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $z_g$ from 0.0 to 0.5.
Data from FigAux 114f. The full covariance matrices for the all-particle $z_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 10 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 10 evenly spaced bins in $z_g$ from 0.0 to 0.5.
Data from FigAux 115d. The full covariance matrices for the all-particle $R_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 6 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 6 bins in $r_g$ (0.06310, 0.10000, 0.15849, 0.25119, 0.39811, 0.63096, 0.80000).
Data from FigAux 115d. The full covariance matrices for the all-particle $R_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 6 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 6 bins in $r_g$ (0.06310, 0.10000, 0.15849, 0.25119, 0.39811, 0.63096, 0.80000).
Data from FigAux 116d. The full covariance matrices for the all-particle $R_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 6 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 6 bins in $r_g$ (0.06310, 0.10000, 0.15849, 0.25119, 0.39811, 0.63096, 0.80000).
Data from FigAux 116d. The full covariance matrices for the all-particle $R_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 6 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 6 bins in $r_g$ (0.06310, 0.10000, 0.15849, 0.25119, 0.39811, 0.63096, 0.80000).
Data from FigAux 115e. The full covariance matrices for the all-particle $R_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 6 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 6 bins in $r_g$ (0.06310, 0.10000, 0.15849, 0.25119, 0.39811, 0.63096, 0.80000).
Data from FigAux 115e. The full covariance matrices for the all-particle $R_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 6 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 6 bins in $r_g$ (0.06310, 0.10000, 0.15849, 0.25119, 0.39811, 0.63096, 0.80000).
Data from FigAux 116e. The full covariance matrices for the all-particle $R_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 6 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 6 bins in $r_g$ (0.06310, 0.10000, 0.15849, 0.25119, 0.39811, 0.63096, 0.80000).
Data from FigAux 116e. The full covariance matrices for the all-particle $R_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 6 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 6 bins in $r_g$ (0.06310, 0.10000, 0.15849, 0.25119, 0.39811, 0.63096, 0.80000).
Data from FigAux 115f. The full covariance matrices for the all-particle $R_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 6 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 6 bins in $r_g$ (0.06310, 0.10000, 0.15849, 0.25119, 0.39811, 0.63096, 0.80000).
Data from FigAux 115f. The full covariance matrices for the all-particle $R_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 6 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 6 bins in $r_g$ (0.06310, 0.10000, 0.15849, 0.25119, 0.39811, 0.63096, 0.80000).
Data from FigAux 116f. The full covariance matrices for the all-particle $R_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 6 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 6 bins in $r_g$ (0.06310, 0.10000, 0.15849, 0.25119, 0.39811, 0.63096, 0.80000).
Data from FigAux 116f. The full covariance matrices for the all-particle $R_g$ distribution for the more forward of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. The distributions are normalized to the integrated cross section, $\sigma$. Each set of 6 bins corresponds to one $p_T$ bin in {300, 400, 600, 800, 1000, infinity } and 6 bins in $r_g$ (0.06310, 0.10000, 0.15849, 0.25119, 0.39811, 0.63096, 0.80000).
Measurements of the spin observables ANN(90∘) and AN0(90∘) for the reaction pp→dπ+ between 500 and 800 MeV are presented and compared with previous measurements and with predictions from theories and a partial-wave analysis. These are the first available measurements of ANN above 590 MeV.
ANALYSING POWER IS POL.POL(NAME=AN0).
We employ data taken by the JADE and OPAL experiments for an integrated QCD study in hadronic e+e- annihilations at c.m.s. energies ranging from 35 GeV through 189 GeV. The study is based on jet-multiplicity related observables. The observables are obtained to high jet resolution scales with the JADE, Durham, Cambridge and cone jet finders, and compared with the predictions of various QCD and Monte Carlo models. The strong coupling strength, alpha_s, is determined at each energy by fits of O(alpha_s^2) calculations, as well as matched O(alpha_s^2) and NLLA predictions, to the data. Matching schemes are compared, and the dependence of the results on the choice of the renormalization scale is investigated. The combination of the results using matched predictions gives alpha_s(MZ)=0.1187+{0.0034}-{0.0019}. The strong coupling is also obtained, at lower precision, from O(alpha_s^2) fits of the c.m.s. energy evolution of some of the observables. A qualitative comparison is made between the data and a recent MLLA prediction for mean jet multiplicities.
Overall result for ALPHAS at the Z0 mass from the combination of the ln R-matching results from the observables evolved using a three-loop running expression. The errors shown are total errors and contain all the statistics and systematics.
Weighted mean for ALPHAS at the Z0 mass determined from the energy evolutions of the mean values of the 2-jet cross sections obtained with the JADE and DURHAMschemes and the 3-jet fraction for the JADE, DURHAM and CAMBRIDGE schemes evaluted at a fixed YCUT.. The errors shown are total errors and contain all the statistics and systematics.
Combined results for ALPHA_S from fits of matched predicitions. The first systematic (DSYS) error is the experimental systematic, the second DSYS error isthe hadronization systematic and the third is the QCD scale error. The values of ALPHAS evolved to the Z0 mass using a three-loop evolution are also given.
Results for ALPHAS from fits of the ln R-matching predictions for the fractional 2-jet rate observable (D2), and the mean jet multiplicities (N) for the Durham and Cambridge schemes. The errors shown are total errors and contain all the statistics and systematics.
Results for ALPHAS at the Z0 mass from fits of the O(alphas**2) predicitonsfor the energy evolution of the mean 2-jet cross section <Y23> for the DURHAM a nd JADE schemes. The errors shown are total errors and contain all the statistics and systematics.
Results for ALPHAS at the Z0 mass from fits of the O(alphas**2) predicitonsfor the 3-jet fractions (R3) for the JADE, DURHAM and CAMBRIDGE schemes. The errors shown are total errors and contain all the statistics and systematics.
N-Jet rates from the JADE collaboration at c.m. energy 35 GeV. Jets define using the JADE/E0 alogrithm.
N-Jet rates from the JADE collaboration at c.m. energy 44 GeV. Jets define using the JADE/E0 alogrithm.
N-Jet rates from the OPAL collaboration at c.m. energy 91 GeV. Jets define using the JADE/E0 alogrithm.
N-Jet rates from the OPAL collaboration at c.m. energy 133 GeV. Jets define using the JADE/E0 alogrithm.
N-Jet rates from the OPAL collaboration at c.m. energy 161 GeV. Jets define using the JADE/E0 alogrithm.
N-Jet rates from the OPAL collaboration at c.m. energy 172 GeV. Jets define using the JADE/E0 alogrithm.
N-Jet rates from the OPAL collaboration at c.m. energy 183 GeV. Jets define using the JADE/E0 alogrithm.
N-Jet rates from the OPAL collaboration at c.m. energy 189 GeV. Jets define using the JADE/E0 alogrithm.
Mean value of the observable Ynm (the value of YCUT at the boundary betweenn and (n+1=m) jets) as a function of the c.m. energy. Data from JADE and OPAL collaborations. Jets defined using the JADE/E0 alogrithm.
N-Jet rates from the JADE collaboration at c.m. energy 35 GeV. Jets defined using the DURHAM alogrithm.
N-Jet rates from the JADE collaboration at c.m. energy 44 GeV. Jets defined using the DURHAM alogrithm.
N-Jet rates from the OPAL collaboration at c.m. energy 91 GeV. Jets defined using the DURHAM alogrithm.
N-Jet rates from the OPAL collaboration at c.m. energy 133 GeV. Jets defined using the DURHAM alogrithm.
N-Jet rates from the OPAL collaboration at c.m. energy 161 GeV. Jets defined using the DURHAM alogrithm.
N-Jet rates from the OPAL collaboration at c.m. energy 172 GeV. Jets defined using the DURHAM alogrithm.
N-Jet rates from the OPAL collaboration at c.m. energy 183 GeV. Jets defined using the DURHAM alogrithm.
N-Jet rates from the OPAL collaboration at c.m. energy 189 GeV. Jets defined using the DURHAM alogrithm.
Differential distributions in Ynm (the minimum YCUT for the separation inton and m(=n+1) jets). ) from the JADE collaboration at c.m. energy 35 GeV. Jets defined using the DURHAM alogrithm.
Differential distributions in Ynm (the minimum YCUT for the separation inton and m(=n+1) jets). ) from the JADE collaboration at c.m. energy 44 GeV. Jets defined using the DURHAM alogrithm.
Differential distributions in Ynm (the minimum YCUT for the separation inton and m(=n+1) jets). ) from the OPAL collaboration at c.m. energy 91 GeV. Jets defined using the DURHAM alogrithm.
Differential distributions in Ynm (the minimum YCUT for the separation inton and m(=n+1) jets). ) from the OPAL collaboration at c.m. energy 133 GeV. Jets defined using the DURHAM alogrithm.
Differential distributions in Ynm (the minimum YCUT for the separation inton and m(=n+1) jets). ) from the OPAL collaboration at c.m. energy 161 GeV. Jets defined using the DURHAM alogrithm.
Differential distributions in Ynm (the minimum YCUT for the separation inton and m(=n+1) jets). ) from the OPAL collaboration at c.m. energy 172 GeV. Jets defined using the DURHAM alogrithm.
Differential distributions in Ynm (the minimum YCUT for the separation inton and m(=n+1) jets). ) from the OPAL collaboration at c.m. energy 183 GeV. Jets defined using the DURHAM alogrithm.
Differential distributions in Ynm (the minimum YCUT for the separation inton and m(=n+1) jets). ) from the OPAL collaboration at c.m. energy 189 GeV. Jets defined using the DURHAM alogrithm.
Mean jet multiplicity as a function of YCUT from the JADE collaboration at c.m. energy 35 GeV. Jets defined using the DURHAM alogrithm.
Mean jet multiplicity as a function of YCUT from the JADE collaboration at c.m. energy 44 GeV. Jets defined using the DURHAM alogrithm.
Mean jet multiplicity as a function of YCUT from the OPAL collaboration at c.m. energy 91 GeV. Jets defined using the DURHAM alogrithm.
Mean jet multiplicity as a function of YCUT from the OPAL collaboration at c.m. energy 133 GeV. Jets defined using the DURHAM alogrithm.
Mean jet multiplicity as a function of YCUT from the OPAL collaboration at c.m. energy 161 GeV. Jets defined using the DURHAM alogrithm.
Mean jet multiplicity as a function of YCUT from the OPAL collaboration at c.m. energy 172 GeV. Jets defined using the DURHAM alogrithm.
Mean jet multiplicity as a function of YCUT from the OPAL collaboration at c.m. energy 183 GeV. Jets defined using the DURHAM alogrithm.
Mean jet multiplicity as a function of YCUT from the OPAL collaboration at c.m. energy 189 GeV. Jets defined using the DURHAM alogrithm.
Mean value of the observable Ynm (the value of YCUT at the boundary betweenn and (n+1=m) jets) as a function of the c.m. energy. Data from JADE and OPAL collaborations. Jets defined using the DURHAM alogrithm.
N-Jet rates from the JADE collaboration at c.m. energy 35 GeV. Jets defined using the CAMBRIDGE alogrithm.
N-Jet rates from the JADE collaboration at c.m. energy 44 GeV. Jets defined using the CAMBRIDGE alogrithm.
N-Jet rates from the OPAL collaboration at c.m. energy 91 GeV. Jets defined using the CAMBRIDGE alogrithm.
N-Jet rates from the OPAL collaboration at c.m. energy 133 GeV. Jets defined using the CAMBRIDGE alogrithm.
N-Jet rates from the OPAL collaboration at c.m. energy 161 GeV. Jets defined using the CAMBRIDGE alogrithm.
N-Jet rates from the OPAL collaboration at c.m. energy 172 GeV. Jets defined using the CAMBRIDGE alogrithm.
N-Jet rates from the OPAL collaboration at c.m. energy 183 GeV. Jets defined using the CAMBRIDGE alogrithm.
N-Jet rates from the OPAL collaboration at c.m. energy 189 GeV. Jets defined using the CAMBRIDGE alogrithm.
Differential N-Jet rates from the JADE collaboration at c.m. energy 35 GeV. Jets defined using the CAMBRIDGE alogrithm.
Differential N-Jet rates from the JADE collaboration at c.m. energy 44 GeV. Jets defined using the CAMBRIDGE alogrithm.
Differential N-Jet rates from the OPAL collaboration at c.m. energy 91 GeV. Jets defined using the CAMBRIDGE alogrithm.
Differential N-Jet rates from the OPAL collaboration at c.m. energy 133 GeV. Jets defined using the CAMBRIDGE alogrithm.
Differential N-Jet rates from the OPAL collaboration at c.m. energy 161 GeV. Jets defined using the CAMBRIDGE alogrithm.
Differential N-Jet rates from the OPAL collaboration at c.m. energy 172 GeV. Jets defined using the CAMBRIDGE alogrithm.
Differential N-Jet rates from the OPAL collaboration at c.m. energy 183 GeV. Jets defined using the CAMBRIDGE alogrithm.
Differential N-Jet rates from the OPAL collaboration at c.m. energy 189 GeV. Jets defined using the CAMBRIDGE alogrithm.
Mean jet multiplicity as a function of YCUT from the JADE collaboration at c.m. energy 35 GeV. Jets defined using the CAMBRIDGE alogrithm.
Mean jet multiplicity as a function of YCUT from the JADE collaboration at c.m. energy 44 GeV. Jets defined using the CAMBRIDGE alogrithm.
Mean jet multiplicity as a function of YCUT from the OPAL collaboration at c.m. energy 91 GeV. Jets defined using the CAMBRIDGE alogrithm.
Mean jet multiplicity as a function of YCUT from the OPAL collaboration at c.m. energy 133 GeV. Jets defined using the CAMBRIDGE alogrithm.
Mean jet multiplicity as a function of YCUT from the OPAL collaboration at c.m. energy 161 GeV. Jets defined using the CAMBRIDGE alogrithm.
Mean jet multiplicity as a function of YCUT from the OPAL collaboration at c.m. energy 172 GeV. Jets defined using the CAMBRIDGE alogrithm.
Mean jet multiplicity as a function of YCUT from the OPAL collaboration at c.m. energy 183 GeV. Jets defined using the CAMBRIDGE alogrithm.
Mean jet multiplicity as a function of YCUT from the OPAL collaboration at c.m. energy 189 GeV. Jets defined using the CAMBRIDGE alogrithm.
N-Jet rates from JADE collaboration at c.m. energy 35 GeV. Jets define using the CONE alogrithm.
N-Jet rates from JADE collaboration at c.m. energy 35 GeV. Jets define using the CONE alogrithm.
N-Jet rates from JADE collaboration at c.m. energy 44 GeV. Jets define using the CONE alogrithm.
N-Jet rates from JADE collaboration at c.m. energy 44 GeV. Jets define using the CONE alogrithm.
N-Jet rates from OPAL collaboration at c.m. energy 91 GeV. Jets define using the CONE alogrithm.
N-Jet rates from OPAL collaboration at c.m. energy 91 GeV. Jets define using the CONE alogrithm.
N-Jet rates from OPAL collaboration at c.m. energy 133 GeV. Jets define using the CONE alogrithm.
N-Jet rates from OPAL collaboration at c.m. energy 133 GeV. Jets define using the CONE alogrithm.
N-Jet rates from OPAL collaboration at c.m. energy 161 GeV. Jets define using the CONE alogrithm.
N-Jet rates from OPAL collaboration at c.m. energy 161 GeV. Jets define using the CONE alogrithm.
N-Jet rates from OPAL collaboration at c.m. energy 172 GeV. Jets define using the CONE alogrithm.
N-Jet rates from OPAL collaboration at c.m. energy 172 GeV. Jets define using the CONE alogrithm.
N-Jet rates from OPAL collaboration at c.m. energy 183 GeV. Jets define using the CONE alogrithm.
N-Jet rates from OPAL collaboration at c.m. energy 183 GeV. Jets define using the CONE alogrithm.
N-Jet rates from OPAL collaboration at c.m. energy 189 GeV. Jets define using the CONE alogrithm.
N-Jet rates from OPAL collaboration at c.m. energy 189 GeV. Jets define using the CONE alogrithm.
Measurements are presented for several mixtures of the spin observables CSS,CSL=CLS, CLL, and CNN for neutron-proton elastic scattering. These data were obtained with a free polarized neutron beam, a polarized proton target, and a large magnetic spectrometer for the outgoing proton. The neutron beam kinetic energies were 484, 567, 634, 720, and 788 MeV. Combining these results with earlier measurements allows the determination of the pure spin observables CSS, CLS, and CLL at 484, 634, and 788 MeV for c.m. angles 25°≤θc.m.≤180° and at 720 MeV for 35°≤θc.m.≤80°. These data make a significant contribution to the knowledge of the isospin-0 nucleon-nucleon scattering amplitudes. © 1996 The American Physical Society.
Results for the pure spin observables. Statistical errors only. (Data for CSS and CNN at (172.5 to 177.5) and (167.5 to 172.5) degrees are uncertain because of the rapid angular dependence and possible errors in angle, and may be omitted from phase shift analyses.) The CNN data without errors are from a phase shift analysis of Arndt et al. (PR D45 (1992) 3395) [FA92] and were used to derive pure spin observables from the measured data.
Results for the pure spin observables. Statistical errors only. (Data for CSS and CNN at (172.5 to 177.5) and (167.5 to 172.5) degrees are uncertain because of the rapid angular dependence and possible errors in angle, and may be omitted from phase shift analyses.) The CNN data without errors are from a phase shift analysis of Arndt et al. (PR D45 (1992) 3395) [FA92] and were used to derive pure spin observables from the measured data.
Results for the pure spin observables. Statistical errors only. The CNN data without errors are from a phase shift analysis of Arndt et al. (PR D45 (1992) 3395) [FA92] and were used to derive pure spin observables from the measured data.
Results for the pure spin observables. Statistical errors only. The CNN data without errors are from a phase shift analysis of Arndt et al. (PR D45 (1992) 3395) [FA92] and were used to derive pure spin observables from the measured data.
Measured values of the mixed spin variables with the coefficients.
Measured values of the mixed spin variables with the coefficients.
Measured values of the mixed spin variables with the coefficients.
Mean values of mixed spin variables with coefficients.
Mean values of mixed spin variables with coefficients.
Mean values of mixed spin variables with coefficients.
Mean values of mixed spin variables with coefficients.
Mean values of mixed spin variables with coefficients.
Mean values of mixed spin variables with coefficients.
Mean values of mixed spin variables with coefficients.
Mean values of mixed spin variables with coefficients.
Mean values of mixed spin variables with coefficients.
Mean values of mixed spin variables with coefficients.
Mean values of mixed spin variables with coefficients.
Mean values of mixed spin variables with coefficients.
We report on a measurement of the ratio of the differential cross sections for W and Z boson production as a function of transverse momentum in proton-antiproton collisions at sqrt(s) = 1.8 TeV. This measurement uses data recorded by the D0 detector at the Fermilab Tevatron in 1994-1995. It represents the first investigation of a proposal that ratios between W and Z observables can be calculated reliably using perturbative QCD, even when the individual observables are not. Using the ratio of differential cross sections reduces both experimental and theoretical uncertainties, and can therefore provide smaller overall uncertainties in the measured mass and width of the W boson than current methods used at hadron colliders.
The measured W and Z0 cross sections used to compute the ratio.
The measured ratios of W+-/Z0 cross sections, corrected for the branching ratios BR(W-->e-nue)=0.1073+-0.0025 and BR(Z0-->E+E-)=0.033632+-0.000059 (PDG 2000). The error given is the total error, but note that the 4.3pct error in the luminosity cancels completely in the ratio.
This paper presents cross sections for the production of a W boson in association with jets, measured in proton--proton collisions at $\sqrt{s}=7$ TeV with the ATLAS experiment at the Large Hadron Collider. With an integrated luminosity of $4.6 fb^{-1}$, this data set allows for an exploration of a large kinematic range, including jet production up to a transverse momentum of 1 TeV and multiplicities up to seven associated jets. The production cross sections for W bosons are measured in both the electron and muon decay channels. Differential cross sections for many observables are also presented including measurements of the jet observables such as the rapidities and the transverse momenta as well as measurements of event observables such as the scalar sums of the transverse momenta of the jets. The measurements are compared to numerous QCD predictions including next-to-leading-order perturbative calculations, resummation calculations and Monte Carlo generators.
Distribution of inclusive jet multiplicity.
Breakdown of systematic uncertainties in percent in inclusive jet multiplicity in the electron channel.Uncertainties have been symmetrised and the sign denotes the sign of the original up-variation.
Breakdown of systematic uncertainties in percent in inclusive jet multiplicity in the muon channel.Uncertainties have been symmetrised and the sign denotes the sign of the original up-variation.
Distribution of exclusive jet multiplicity.
Breakdown of systematic uncertainties in percent in exclusive jet multiplicity in the electron channel.Uncertainties have been symmetrised and the sign denotes the sign of the original up-variation.
Breakdown of systematic uncertainties in percent in exclusive jet multiplicity in the muon channel.Uncertainties have been symmetrised and the sign denotes the sign of the original up-variation.
Distribution of pT (leading jet) [GeV] with at least one jet in the event.
Breakdown of systematic uncertainties in percent in pT (leading jet) [GeV] with at least one jet in the event in the electron channel.Uncertainties have been symmetrised and the sign denotes the sign of the original up-variation.
Breakdown of systematic uncertainties in percent in pT (leading jet) [GeV] with at least one jet in the event in the muon channel.Uncertainties have been symmetrised and the sign denotes the sign of the original up-variation.
Distribution of pT (leading jet) [GeV] with exactly one jet in the event.
Breakdown of systematic uncertainties in percent in pT (leading jet) [GeV] with exactly one jet in the event in the electron channel.Uncertainties have been symmetrised and the sign denotes the sign of the original up-variation.
Breakdown of systematic uncertainties in percent in pT (leading jet) [GeV] with exactly one jet in the event in the muon channel.Uncertainties have been symmetrised and the sign denotes the sign of the original up-variation.
Distribution of pT (leading jet) [GeV] with at least two jets in the event.
Breakdown of systematic uncertainties in percent in pT (leading jet) [GeV] with at least two jets in the event in the electron channel.Uncertainties have been symmetrised and the sign denotes the sign of the original up-variation.
Breakdown of systematic uncertainties in percent in pT (leading jet) [GeV] with at least two jets in the event in the muon channel.Uncertainties have been symmetrised and the sign denotes the sign of the original up-variation.
Distribution of pT (leading jet) [GeV] with at least three jets in the event.
Breakdown of systematic uncertainties in percent in pT (leading jet) [GeV] with at least three jets in the event in the electron channel.Uncertainties have been symmetrised and the sign denotes the sign of the original up-variation.
Breakdown of systematic uncertainties in percent in pT (leading jet) [GeV] with at least three jets in the event in the muon channel.Uncertainties have been symmetrised and the sign denotes the sign of the original up-variation.
Distribution of pT (2nd jet) [GeV] with at least two jets in the event.
Breakdown of systematic uncertainties in percent in pT (2nd jet) [GeV] with at least two jets in the event in the electron channel.Uncertainties have been symmetrised and the sign denotes the sign of the original up-variation.
Breakdown of systematic uncertainties in percent in pT (2nd jet) [GeV] with at least two jets in the event in the muon channel.Uncertainties have been symmetrised and the sign denotes the sign of the original up-variation.
Distribution of pT (3rd jet) [GeV] with at least three jets in the event.
Breakdown of systematic uncertainties in percent in pT (3rd jet) [GeV] with at least three jets in the event in the electron channel.Uncertainties have been symmetrised and the sign denotes the sign of the original up-variation.
Breakdown of systematic uncertainties in percent in pT (3rd jet) [GeV] with at least three jets in the event in the muon channel.Uncertainties have been symmetrised and the sign denotes the sign of the original up-variation.
Distribution of pT (4th jet) [GeV] with at least four jets in the event.
Breakdown of systematic uncertainties in percent in pT (4th jet) [GeV] with at least four jets in the event in the electron channel.Uncertainties have been symmetrised and the sign denotes the sign of the original up-variation.
Breakdown of systematic uncertainties in percent in pT (4th jet) [GeV] with at least four jets in the event in the muon channel.Uncertainties have been symmetrised and the sign denotes the sign of the original up-variation.
Distribution of pT (5th jet) [GeV] with at least five jets in the event.
Breakdown of systematic uncertainties in percent in pT (5th jet) [GeV] with at least five jets in the event in the electron channel.Uncertainties have been symmetrised and the sign denotes the sign of the original up-variation.
Breakdown of systematic uncertainties in percent in pT (5th jet) [GeV] with at least five jets in the event in the muon channel.Uncertainties have been symmetrised and the sign denotes the sign of the original up-variation.
Distribution of leading jet rapidity with at least one jet in the event.
Breakdown of systematic uncertainties in percent in leading jet rapidity with at least one jet in the event in the electron channel.Uncertainties have been symmetrised and the sign denotes the sign of the original up-variation.
Breakdown of systematic uncertainties in percent in leading jet rapidity with at least one jet in the event in the muon channel.Uncertainties have been symmetrised and the sign denotes the sign of the original up-variation.
Distribution of 2nd jet rapidity with at least two jets in the event.
Breakdown of systematic uncertainties in percent in 2nd jet rapidity with at least two jets in the event in the electron channel.Uncertainties have been symmetrised and the sign denotes the sign of the original up-variation.
Breakdown of systematic uncertainties in percent in 2nd jet rapidity with at least two jets in the event in the muon channel.Uncertainties have been symmetrised and the sign denotes the sign of the original up-variation.
Distribution of HT [GeV] with at least one jet in the event.
Breakdown of systematic uncertainties in percent in HT [GeV] with at least one jet in the event in the electron channel.Uncertainties have been symmetrised and the sign denotes the sign of the original up-variation.
Breakdown of systematic uncertainties in percent in HT [GeV] with at least one jet in the event in the muon channel.Uncertainties have been symmetrised and the sign denotes the sign of the original up-variation.
Distribution of HT [GeV] with exactly one jet in the event.
Breakdown of systematic uncertainties in percent in HT [GeV] with exactly one jet in the event in the electron channel.Uncertainties have been symmetrised and the sign denotes the sign of the original up-variation.
Breakdown of systematic uncertainties in percent in HT [GeV] with exactly one jet in the event in the muon channel.Uncertainties have been symmetrised and the sign denotes the sign of the original up-variation.
Distribution of HT [GeV] with at least two jets in the event.
Breakdown of systematic uncertainties in percent in HT [GeV] with at least two jets in the event in the electron channel.Uncertainties have been symmetrised and the sign denotes the sign of the original up-variation.
Breakdown of systematic uncertainties in percent in HT [GeV] with at least two jets in the event in the muon channel.Uncertainties have been symmetrised and the sign denotes the sign of the original up-variation.
Distribution of HT [GeV] with exactly two jets in the event.
Breakdown of systematic uncertainties in percent in HT [GeV] with exactly two jets in the event in the electron channel.Uncertainties have been symmetrised and the sign denotes the sign of the original up-variation.
Breakdown of systematic uncertainties in percent in HT [GeV] with exactly two jets in the event in the muon channel.Uncertainties have been symmetrised and the sign denotes the sign of the original up-variation.
Distribution of HT [GeV] with at least three jets in the event.
Breakdown of systematic uncertainties in percent in HT [GeV] with at least three jets in the event in the electron channel.Uncertainties have been symmetrised and the sign denotes the sign of the original up-variation.
Breakdown of systematic uncertainties in percent in HT [GeV] with at least three jets in the event in the muon channel.Uncertainties have been symmetrised and the sign denotes the sign of the original up-variation.
Distribution of HT [GeV] with exactly three jets in the event.
Breakdown of systematic uncertainties in percent in HT [GeV] with exactly three jets in the event in the electron channel.Uncertainties have been symmetrised and the sign denotes the sign of the original up-variation.
Breakdown of systematic uncertainties in percent in HT [GeV] with exactly three jets in the event in the muon channel.Uncertainties have been symmetrised and the sign denotes the sign of the original up-variation.
Distribution of HT [GeV] with at least four jets in the event.
Breakdown of systematic uncertainties in percent in HT [GeV] with at least four jets in the event in the electron channel.Uncertainties have been symmetrised and the sign denotes the sign of the original up-variation.
Breakdown of systematic uncertainties in percent in HT [GeV] with at least four jets in the event in the muon channel.Uncertainties have been symmetrised and the sign denotes the sign of the original up-variation.
Distribution of HT [GeV] with at least five jets in the event.
Breakdown of systematic uncertainties in percent in HT [GeV] with at least five jets in the event in the electron channel.Uncertainties have been symmetrised and the sign denotes the sign of the original up-variation.
Breakdown of systematic uncertainties in percent in HT [GeV] with at least five jets in the event in the muon channel.Uncertainties have been symmetrised and the sign denotes the sign of the original up-variation.
Distribution of DPhi(jj) [GeV] with at least two jets in the event.
Breakdown of systematic uncertainties in percent in DPhi(jj) [GeV] with at least two jets in the event in the electron channel.Uncertainties have been symmetrised and the sign denotes the sign of the original up-variation.
Breakdown of systematic uncertainties in percent in DPhi(jj) [GeV] with at least two jets in the event in the muon channel.Uncertainties have been symmetrised and the sign denotes the sign of the original up-variation.
Distribution of Dy(jj) [GeV] with at least two jets in the event.
Breakdown of systematic uncertainties in percent in Dy(jj) [GeV] with at least two jets in the event in the electron channel.Uncertainties have been symmetrised and the sign denotes the sign of the original up-variation.
Breakdown of systematic uncertainties in percent in Dy(jj) [GeV] with at least two jets in the event in the muon channel.Uncertainties have been symmetrised and the sign denotes the sign of the original up-variation.
Distribution of DR(jj) [GeV] with at least two jets in the event.
Breakdown of systematic uncertainties in percent in DR(jj) [GeV] with at least two jets in the event in the electron channel.Uncertainties have been symmetrised and the sign denotes the sign of the original up-variation.
Breakdown of systematic uncertainties in percent in DR(jj) [GeV] with at least two jets in the event in the muon channel.Uncertainties have been symmetrised and the sign denotes the sign of the original up-variation.
Distribution of m(jj) [GeV] with at least two jets in the event.
Breakdown of systematic uncertainties in percent in m(jj) [GeV] with at least two jets in the event in the electron channel.Uncertainties have been symmetrised and the sign denotes the sign of the original up-variation.
Breakdown of systematic uncertainties in percent in m(jj) [GeV] with at least two jets in the event in the muon channel.Uncertainties have been symmetrised and the sign denotes the sign of the original up-variation.
Distribution of 3rd jet rapidity with at least three jets in the event.
Breakdown of systematic uncertainties in percent in 3rd jet rapidity with at least three jets in the event in the electron channel.Uncertainties have been symmetrised and the sign denotes the sign of the original up-variation.
Breakdown of systematic uncertainties in percent in 3rd jet rapidity with at least three jets in the event in the muon channel.Uncertainties have been symmetrised and the sign denotes the sign of the original up-variation.
Distribution of 4th jet rapidity with at least four jets in the event.
Breakdown of systematic uncertainties in percent in 4th jet rapidity with at least four jets in the event in the electron channel.Uncertainties have been symmetrised and the sign denotes the sign of the original up-variation.
Breakdown of systematic uncertainties in percent in 4th jet rapidity with at least four jets in the event in the muon channel.Uncertainties have been symmetrised and the sign denotes the sign of the original up-variation.
Distribution of 5th jet rapidity with at least five jets in the event.
Breakdown of systematic uncertainties in percent in 5th jet rapidity with at least five jets in the event in the electron channel.Uncertainties have been symmetrised and the sign denotes the sign of the original up-variation.
Breakdown of systematic uncertainties in percent in 5th jet rapidity with at least five jets in the event in the muon channel.Uncertainties have been symmetrised and the sign denotes the sign of the original up-variation.
Distribution of ST [GeV] with at least one jet in the event.
Breakdown of systematic uncertainties in percent in ST [GeV] with at least one jet in the event in the electron channel.Uncertainties have been symmetrised and the sign denotes the sign of the original up-variation.
Breakdown of systematic uncertainties in percent in ST [GeV] with at least one jet in the event in the muon channel.Uncertainties have been symmetrised and the sign denotes the sign of the original up-variation.
Distribution of ST [GeV] with at least two jets in the event.
Breakdown of systematic uncertainties in percent in ST [GeV] with at least two jets in the event in the electron channel.Uncertainties have been symmetrised and the sign denotes the sign of the original up-variation.
Breakdown of systematic uncertainties in percent in ST [GeV] with at least two jets in the event in the muon channel.Uncertainties have been symmetrised and the sign denotes the sign of the original up-variation.
Distribution of ST [GeV] with exactly two jets in the event.
Breakdown of systematic uncertainties in percent in ST [GeV] with exactly two jets in the event in the electron channel.Uncertainties have been symmetrised and the sign denotes the sign of the original up-variation.
Breakdown of systematic uncertainties in percent in ST [GeV] with exactly two jets in the event in the muon channel.Uncertainties have been symmetrised and the sign denotes the sign of the original up-variation.
Distribution of ST [GeV] with at least three jets in the event.
Breakdown of systematic uncertainties in percent in ST [GeV] with at least three jets in the event in the electron channel.Uncertainties have been symmetrised and the sign denotes the sign of the original up-variation.
Breakdown of systematic uncertainties in percent in ST [GeV] with at least three jets in the event in the muon channel.Uncertainties have been symmetrised and the sign denotes the sign of the original up-variation.
Distribution of ST [GeV] with exactly three jets in the event.
Breakdown of systematic uncertainties in percent in ST [GeV] with exactly three jets in the event in the electron channel.Uncertainties have been symmetrised and the sign denotes the sign of the original up-variation.
Breakdown of systematic uncertainties in percent in ST [GeV] with exactly three jets in the event in the muon channel.Uncertainties have been symmetrised and the sign denotes the sign of the original up-variation.
Distribution of ST [GeV] with at least four jets in the event.
Breakdown of systematic uncertainties in percent in ST [GeV] with at least four jets in the event in the electron channel.Uncertainties have been symmetrised and the sign denotes the sign of the original up-variation.
Breakdown of systematic uncertainties in percent in ST [GeV] with at least four jets in the event in the muon channel.Uncertainties have been symmetrised and the sign denotes the sign of the original up-variation.
Distribution of ST [GeV] with at least five jets in the event.
Breakdown of systematic uncertainties in percent in ST [GeV] with at least five jets in the event in the electron channel.Uncertainties have been symmetrised and the sign denotes the sign of the original up-variation.
Breakdown of systematic uncertainties in percent in ST [GeV] with at least five jets in the event in the muon channel.Uncertainties have been symmetrised and the sign denotes the sign of the original up-variation.
We present a measurement of angular observables, $P_4'$, $P_5'$, $P_6'$, $P_8'$, in the decay $B^0 \to K^\ast(892)^0 \ell^+ \ell^-$, where $\ell^+\ell^-$ is either $e^+e^-$ or $\mu^+\mu^-$. The analysis is performed on a data sample corresponding to an integrated luminosity of $711~\mathrm{fb}^{-1}$ containing $772\times 10^{6}$ $B\bar B$ pairs, collected at the $\Upsilon(4S)$ resonance with the Belle detector at the asymmetric-energy $e^+e^-$ collider KEKB. Four angular observables, $P_{4,5,6,8}'$ are extracted in five bins of the invariant mass squared of the lepton system, $q^2$. We compare our results for $P_{4,5,6,8}'$ with Standard Model predictions including the $q^2$ region in which the LHCb collaboration reported the so-called $P_5'$ anomaly.
Results of the angular analysis of $B^0 \to K^\ast(892)^0 \ell^+ \ell^-$ (where $\ell = e,\mu$) in five bins of $q^2$, the di-lepton invariant mass squared.
Event-shape observables measured using charged particles in inclusive $Z$-boson events are presented, using the electron and muon decay modes of the $Z$ bosons. The measurements are based on an integrated luminosity of $1.1 {\rm fb}^{-1}$ of proton--proton collisions recorded by the ATLAS detector at the LHC at a centre-of-mass energy $\sqrt{s}=7$ TeV. Charged-particle distributions, excluding the lepton--antilepton pair from the $Z$-boson decay, are measured in different ranges of transverse momentum of the $Z$ boson. Distributions include multiplicity, scalar sum of transverse momenta, beam thrust, transverse thrust, spherocity, and $\mathcal{F}$-parameter, which are in particular sensitive to properties of the underlying event at small values of the $Z$-boson transverse momentum. The Sherpa event generator shows larger deviations from the measured observables than Pythia8 and Herwig7. Typically, all three Monte Carlo generators provide predictions that are in better agreement with the data at high $Z$-boson transverse momenta than at low $Z$-boson transverse momenta and for the observables that are less sensitive to the number of charged particles in the event.
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The spin correlation parameters$A_{oonn}, A_{ooss}, A_{oosk}, A_{ookk}$and the analyzing power$A_{oono}$have been measured i
Measurement of the analysing power. Statistical errors only are shown. For the systematic errors see the systematics section above. Note that there are two overlapping angular settings.
Measurements of the spin correlation parameter CNN. Statistical errors onlyare shown. For the systematics see the systematic section above. Note the two overlapping angular settings.
Measurements of the spin correlation parameter CLL. Statistical errors onlyare shown. For the systematics see the systematic section above. Note the two overlapping angular settings.
Measurements of the combined spin observable Cpq measured in the (x,xz) position as a linear combination of CSS, CSL and CLL (see the table above for the coefficients). The errors are purely statistical. An extra 6 PCT uncertainty has to be added to the systematic errors shown in the systematic section above.
Measurements of the combined spin observable Cpq measured in the (x,z) position as a linear combination of CSL and CLL (see the table above for the coefficients). The errors are purely statistical. An extra 6 PCT uncertainty has to be added to the systematic errors shown in the systematic section above.
The measurements of the inclusive and differential fiducial cross sections of the Higgs boson decaying to a pair of photons are presented. The analysis is performed using proton-proton collisions data recorded with the CMS detector at the LHC at a centre-of-mass energy of 13 TeV and corresponding to an integrated luminosity of 137 fb$^{-1}$. The inclusive fiducial cross section is measured to be $\sigma_\mathrm{fid}$ = 73.4 $_{-5.3}^{+5.4}$ (stat) ${}_{-2.2}^{+2.4}$ (syst) fb, in agreement with the standard model expectation of 75.4 $\pm$ 4.1 fb. The measurements are also performed in fiducial regions targeting different production modes and as function of several observables describing the diphoton system, the number of additional jets present in the event, and other kinematic observables. Two double differential measurements are performed. No significant deviations from the standard model expectations are observed.
Differential fiducial higgs to diphoton cross section with respect to $p_{\mathrm{T}}^{\gamma\gamma}$. The last bin in the differential observable extends to infinity and the measured fiducial cross section in this bin is devided by the given bin width
Differential fiducial higgs to diphoton cross section with respect to $p_{\mathrm{T}}^{\gamma\gamma}$. The last bin in the differential observable extends to infinity and the measured fiducial cross section in this bin is devided by the given bin width
Correlation between the measured fiducial cross sections in the different bins of $p_{\mathrm{T}}^{\gamma\gamma}$
Correlation between the measured fiducial cross sections in the different bins of $p_{\mathrm{T}}^{\gamma\gamma}$
Differential fiducial higgs to diphoton cross section with respect to $n_{\mathrm{jets}}$
Differential fiducial higgs to diphoton cross section with respect to $n_{\mathrm{jets}}$
Correlation between the measured fiducial cross sections in the different bins of $n_{\mathrm{jets}}$
Correlation between the measured fiducial cross sections in the different bins of $n_{\mathrm{jets}}$
Differential fiducial higgs to diphoton cross section with respect to $\left|\cos\theta^{\ast}\right|$
Differential fiducial higgs to diphoton cross section with respect to $\left|\cos\theta^{\ast}\right|$
Correlation between the measured fiducial cross sections in the different bins of $\left|\cos\theta^{\ast}\right|$
Correlation between the measured fiducial cross sections in the different bins of $\left|\cos\theta^{\ast}\right|$
Differential fiducial higgs to diphoton cross section with respect to $\left|y^{\gamma\gamma}\right|$
Differential fiducial higgs to diphoton cross section with respect to $\left|y^{\gamma\gamma}\right|$
Correlation between the measured fiducial cross sections in the different bins of $\left|y^{\gamma\gamma}\right|$
Correlation between the measured fiducial cross sections in the different bins of $\left|y^{\gamma\gamma}\right|$
Differential fiducial higgs to diphoton cross section with respect to $p_{\mathrm{T}}^{j_{1}}$. The last bin in the differential observable extends to infinity and the measured fiducial cross section in this bin is devided by the given bin width
Differential fiducial higgs to diphoton cross section with respect to $p_{\mathrm{T}}^{j_{1}}$. The last bin in the differential observable extends to infinity and the measured fiducial cross section in this bin is devided by the given bin width
Correlation between the measured fiducial cross sections in the different bins of $p_{\mathrm{T}}^{j_{1}}$
Correlation between the measured fiducial cross sections in the different bins of $p_{\mathrm{T}}^{j_{1}}$
Differential fiducial higgs to diphoton cross section with respect to $\left|y^{j_{1}}\right|$
Differential fiducial higgs to diphoton cross section with respect to $\left|y^{j_{1}}\right|$
Correlation between the measured fiducial cross sections in the different bins of $\left|y^{j_{1}}\right|$
Correlation between the measured fiducial cross sections in the different bins of $\left|y^{j_{1}}\right|$
Differential fiducial higgs to diphoton cross section with respect to $\left|\Delta y_{\gamma\gamma,j_{1}}\right|$. The last bin in the differential observable extends to infinity and the measured fiducial cross section in this bin is devided by the given bin width
Differential fiducial higgs to diphoton cross section with respect to $\left|\Delta y_{\gamma\gamma,j_{1}}\right|$. The last bin in the differential observable extends to infinity and the measured fiducial cross section in this bin is devided by the given bin width
Correlation between the measured fiducial cross sections in the different bins of $\left|\Delta y_{\gamma\gamma,j_{1}}\right|$
Correlation between the measured fiducial cross sections in the different bins of $\left|\Delta y_{\gamma\gamma,j_{1}}\right|$
Differential fiducial higgs to diphoton cross section with respect to $\left|\Delta\phi_{\gamma\gamma,j_{1}}\right|$
Differential fiducial higgs to diphoton cross section with respect to $\left|\Delta\phi_{\gamma\gamma,j_{1}}\right|$
Correlation between the measured fiducial cross sections in the different bins of $\left|\Delta\phi_{\gamma\gamma,j_{1}}\right|$
Correlation between the measured fiducial cross sections in the different bins of $\left|\Delta\phi_{\gamma\gamma,j_{1}}\right|$
Differential fiducial higgs to diphoton cross section with respect to $p_{\mathrm{T}}^{j_{2}}$. The last bin in the differential observable extends to infinity and the measured fiducial cross section in this bin is devided by the given bin width
Differential fiducial higgs to diphoton cross section with respect to $p_{\mathrm{T}}^{j_{2}}$. The last bin in the differential observable extends to infinity and the measured fiducial cross section in this bin is devided by the given bin width
Correlation between the measured fiducial cross sections in the different bins of $p_{\mathrm{T}}^{j_{2}}$
Correlation between the measured fiducial cross sections in the different bins of $p_{\mathrm{T}}^{j_{2}}$
Differential fiducial higgs to diphoton cross section with respect to $\left|y^{j_{2}}\right|$
Differential fiducial higgs to diphoton cross section with respect to $\left|y^{j_{2}}\right|$
Correlation between the measured fiducial cross sections in the different bins of $\left|y^{j_{2}}\right|$
Correlation between the measured fiducial cross sections in the different bins of $\left|y^{j_{2}}\right|$
Differential fiducial higgs to diphoton cross section with respect to $|\Delta\phi_{\gamma\gamma,j_{1}j_{2}}|$
Differential fiducial higgs to diphoton cross section with respect to $|\Delta\phi_{\gamma\gamma,j_{1}j_{2}}|$
Correlation between the measured fiducial cross sections in the different bins of $|\Delta\phi_{\gamma\gamma,j_{1}j_{2}}|$
Correlation between the measured fiducial cross sections in the different bins of $|\Delta\phi_{\gamma\gamma,j_{1}j_{2}}|$
Differential fiducial higgs to diphoton cross section with respect to $|\Delta\phi_{j_{1},j_{2}}|$
Differential fiducial higgs to diphoton cross section with respect to $|\Delta\phi_{j_{1},j_{2}}|$
Correlation between the measured fiducial cross sections in the different bins of $|\Delta\phi_{j_{1},j_{2}}|$
Correlation between the measured fiducial cross sections in the different bins of $|\Delta\phi_{j_{1},j_{2}}|$
Differential fiducial higgs to diphoton cross section with respect to $|\bar{\eta}_{j_{1},j_{2}}-\eta_{\gamma\gamma}|$. The last bin in the differential observable extends to infinity and the measured fiducial cross section in this bin is devided by the given bin width
Differential fiducial higgs to diphoton cross section with respect to $|\bar{\eta}_{j_{1},j_{2}}-\eta_{\gamma\gamma}|$. The last bin in the differential observable extends to infinity and the measured fiducial cross section in this bin is devided by the given bin width
Correlation between the measured fiducial cross sections in the different bins of $|\bar{\eta}_{j_{1},j_{2}}-\eta_{\gamma\gamma}|$
Correlation between the measured fiducial cross sections in the different bins of $|\bar{\eta}_{j_{1},j_{2}}-\eta_{\gamma\gamma}|$
Differential fiducial higgs to diphoton cross section with respect to $m_{\mathrm{jj}}$. The last bin in the differential observable extends to infinity and the measured fiducial cross section in this bin is devided by the given bin width
Differential fiducial higgs to diphoton cross section with respect to $m_{\mathrm{jj}}$. The last bin in the differential observable extends to infinity and the measured fiducial cross section in this bin is devided by the given bin width
Correlation between the measured fiducial cross sections in the different bins of $m_{\mathrm{jj}}$
Correlation between the measured fiducial cross sections in the different bins of $m_{\mathrm{jj}}$
Differential fiducial higgs to diphoton cross section with respect to $|\Delta\eta_{j_{1},j_{2}}|$. The last bin in the differential observable extends to infinity and the measured fiducial cross section in this bin is devided by the given bin width
Differential fiducial higgs to diphoton cross section with respect to $|\Delta\eta_{j_{1},j_{2}}|$. The last bin in the differential observable extends to infinity and the measured fiducial cross section in this bin is devided by the given bin width
Correlation between the measured fiducial cross sections in the different bins of $|\Delta\eta_{j_{1},j_{2}}|$
Correlation between the measured fiducial cross sections in the different bins of $|\Delta\eta_{j_{1},j_{2}}|$
Differential fiducial higgs to diphoton cross section with respect to $n_{\mathrm{leptons}}$
Differential fiducial higgs to diphoton cross section with respect to $n_{\mathrm{leptons}}$
Correlation between the measured fiducial cross sections in the different bins of $n_{\mathrm{leptons}}$
Correlation between the measured fiducial cross sections in the different bins of $n_{\mathrm{leptons}}$
Differential fiducial higgs to diphoton cross section with respect to $n_{\mathrm{b-jets}}$
Differential fiducial higgs to diphoton cross section with respect to $n_{\mathrm{b-jets}}$
Correlation between the measured fiducial cross sections in the different bins of $n_{\mathrm{b-jets}}$
Correlation between the measured fiducial cross sections in the different bins of $n_{\mathrm{b-jets}}$
Differential fiducial higgs to diphoton cross section with respect to $p_{\mathrm{T}}^{\mathrm{miss}}$. The last bin in the differential observable extends to infinity and the measured fiducial cross section in this bin is devided by the given bin width
Differential fiducial higgs to diphoton cross section with respect to $p_{\mathrm{T}}^{\mathrm{miss}}$. The last bin in the differential observable extends to infinity and the measured fiducial cross section in this bin is devided by the given bin width
Correlation between the measured fiducial cross sections in the different bins of $p_{\mathrm{T}}^{\mathrm{miss}}$
Correlation between the measured fiducial cross sections in the different bins of $p_{\mathrm{T}}^{\mathrm{miss}}$
Differential fiducial higgs to diphoton cross section with respect to $p_{\mathrm{T}}^{j_{2}}$ in the VBF enriched PS. The last bin in the differential observable extends to infinity and the measured fiducial cross section in this bin is devided by the given bin width
Differential fiducial higgs to diphoton cross section with respect to $p_{\mathrm{T}}^{j_{2}}$ in the VBF enriched PS. The last bin in the differential observable extends to infinity and the measured fiducial cross section in this bin is devided by the given bin width
Correlation between the measured fiducial cross sections in the different bins of $p_{\mathrm{T}}^{j_{2}}$
Correlation between the measured fiducial cross sections in the different bins of $p_{\mathrm{T}}^{j_{2}}$
Differential fiducial higgs to diphoton cross section with respect to $|\Delta\phi_{\gamma\gamma,j_{1}j_{2}}|$ in the VBF enriched PS
Differential fiducial higgs to diphoton cross section with respect to $|\Delta\phi_{\gamma\gamma,j_{1}j_{2}}|$ in the VBF enriched PS
Correlation between the measured fiducial cross sections in the different bins of $|\Delta\phi_{\gamma\gamma,j_{1}j_{2}}|$
Correlation between the measured fiducial cross sections in the different bins of $|\Delta\phi_{\gamma\gamma,j_{1}j_{2}}|$
Differential fiducial higgs to diphoton cross section with respect to $|\Delta\phi_{j_{1},j_{2}}|$ in the VBF enriched PS
Differential fiducial higgs to diphoton cross section with respect to $|\Delta\phi_{j_{1},j_{2}}|$ in the VBF enriched PS
Correlation between the measured fiducial cross sections in the different bins of $|\Delta\phi_{j_{1},j_{2}}|$
Correlation between the measured fiducial cross sections in the different bins of $|\Delta\phi_{j_{1},j_{2}}|$
Differential fiducial higgs to diphoton cross section with respect to $p_{\mathrm{T}}^{\gamma\gamma}$ in the VBF enriched PS. The last bin in the differential observable extends to infinity and the measured fiducial cross section in this bin is devided by the given bin width
Differential fiducial higgs to diphoton cross section with respect to $p_{\mathrm{T}}^{\gamma\gamma}$ in the VBF enriched PS. The last bin in the differential observable extends to infinity and the measured fiducial cross section in this bin is devided by the given bin width
Correlation between the measured fiducial cross sections in the different bins of $p_{\mathrm{T}}^{\gamma\gamma}$
Correlation between the measured fiducial cross sections in the different bins of $p_{\mathrm{T}}^{\gamma\gamma}$
Differential fiducial higgs to diphoton cross section with respect to $\tau_{\mathrm{C}}^{j}$. The last bin in the differential observable extends to infinity and the measured fiducial cross section in this bin is devided by the given bin width
Differential fiducial higgs to diphoton cross section with respect to $\tau_{\mathrm{C}}^{j}$. The last bin in the differential observable extends to infinity and the measured fiducial cross section in this bin is devided by the given bin width
Correlation between the measured fiducial cross sections in the different bins of $\tau_{\mathrm{C}}^{j}$
Correlation between the measured fiducial cross sections in the different bins of $\tau_{\mathrm{C}}^{j}$
Differential fiducial higgs to diphoton cross section with respect to $\left|\phi_{\eta}^{\ast}\right|$. The last bin in the differential observable extends to infinity and the measured fiducial cross section in this bin is devided by the given bin width
Differential fiducial higgs to diphoton cross section with respect to $\left|\phi_{\eta}^{\ast}\right|$. The last bin in the differential observable extends to infinity and the measured fiducial cross section in this bin is devided by the given bin width
Correlation between the measured fiducial cross sections in the different bins of $\left|\phi_{\eta}^{\ast}\right|$
Correlation between the measured fiducial cross sections in the different bins of $\left|\phi_{\eta}^{\ast}\right|$
Differential fiducial higgs to diphoton cross section with respect to $p_{\mathrm{T}}^{\gamma\gamma}$ vs. $\tau_{\mathrm{C}}^{j}$. The last bin in the differential observable extends to infinity and the measured fiducial cross section in this bin is devided by the given bin width
Differential fiducial higgs to diphoton cross section with respect to $p_{\mathrm{T}}^{\gamma\gamma}$ vs. $\tau_{\mathrm{C}}^{j}$. The last bin in the differential observable extends to infinity and the measured fiducial cross section in this bin is devided by the given bin width
Differential fiducial higgs to diphoton cross section with respect to $p_{\mathrm{T}}^{\gamma\gamma}$ vs. $\tau_{\mathrm{C}}^{j}$. The last bin in the differential observable extends to infinity and the measured fiducial cross section in this bin is devided by the given bin width
Differential fiducial higgs to diphoton cross section with respect to $p_{\mathrm{T}}^{\gamma\gamma}$ vs. $\tau_{\mathrm{C}}^{j}$. The last bin in the differential observable extends to infinity and the measured fiducial cross section in this bin is devided by the given bin width
Differential fiducial higgs to diphoton cross section with respect to $p_{\mathrm{T}}^{\gamma\gamma}$ vs. $\tau_{\mathrm{C}}^{j}$. The last bin in the differential observable extends to infinity and the measured fiducial cross section in this bin is devided by the given bin width
Differential fiducial higgs to diphoton cross section with respect to $p_{\mathrm{T}}^{\gamma\gamma}$ vs. $\tau_{\mathrm{C}}^{j}$. The last bin in the differential observable extends to infinity and the measured fiducial cross section in this bin is devided by the given bin width
Differential fiducial higgs to diphoton cross section with respect to $p_{\mathrm{T}}^{\gamma\gamma}$ vs. $\tau_{\mathrm{C}}^{j}$. The last bin in the differential observable extends to infinity and the measured fiducial cross section in this bin is devided by the given bin width
Differential fiducial higgs to diphoton cross section with respect to $p_{\mathrm{T}}^{\gamma\gamma}$ vs. $\tau_{\mathrm{C}}^{j}$. The last bin in the differential observable extends to infinity and the measured fiducial cross section in this bin is devided by the given bin width
Correlation between the measured fiducial cross sections in the different bins of $p_{\mathrm{T}}^{\gamma\gamma}$ and $\tau_{\mathrm{C}}^{j}$
Correlation between the measured fiducial cross sections in the different bins of $p_{\mathrm{T}}^{\gamma\gamma}$ and $\tau_{\mathrm{C}}^{j}$
Differential fiducial higgs to diphoton cross section with respect to $p_{\mathrm{T}}^{\gamma\gamma}$ vs. $n_{\mathrm{jets}}$. The last bin in the differential observable extends to infinity and the measured fiducial cross section in this bin is devided by the given bin width
Differential fiducial higgs to diphoton cross section with respect to $p_{\mathrm{T}}^{\gamma\gamma}$ vs. $n_{\mathrm{jets}}$. The last bin in the differential observable extends to infinity and the measured fiducial cross section in this bin is devided by the given bin width
Differential fiducial higgs to diphoton cross section with respect to $p_{\mathrm{T}}^{\gamma\gamma}$ vs. $n_{\mathrm{jets}}$. The last bin in the differential observable extends to infinity and the measured fiducial cross section in this bin is devided by the given bin width
Differential fiducial higgs to diphoton cross section with respect to $p_{\mathrm{T}}^{\gamma\gamma}$ vs. $n_{\mathrm{jets}}$. The last bin in the differential observable extends to infinity and the measured fiducial cross section in this bin is devided by the given bin width
Differential fiducial higgs to diphoton cross section with respect to $p_{\mathrm{T}}^{\gamma\gamma}$ vs. $n_{\mathrm{jets}}$. The last bin in the differential observable extends to infinity and the measured fiducial cross section in this bin is devided by the given bin width
Differential fiducial higgs to diphoton cross section with respect to $p_{\mathrm{T}}^{\gamma\gamma}$ vs. $n_{\mathrm{jets}}$. The last bin in the differential observable extends to infinity and the measured fiducial cross section in this bin is devided by the given bin width
Correlation between the measured fiducial cross sections in the different bins of $p_{\mathrm{T}}^{\gamma\gamma}$ and $n_{\mathrm{jets}}$
Correlation between the measured fiducial cross sections in the different bins of $p_{\mathrm{T}}^{\gamma\gamma}$ and $n_{\mathrm{jets}}$
Results are presented from a search for CP violation in top quark pair production, using proton-proton collisions at a center-of-mass energy of 13 TeV. The data used for this analysis consist of final states with two charged leptons collected by the CMS experiment, and correspond to an integrated luminosity of 35.9 fb$^{-1}$. The search uses two observables, $\mathcal{O}_1$ and $\mathcal{O}_3$, which are Lorentz scalars. The observable $\mathcal{O}_1$ is constructed from the four-momenta of the charged leptons and the reconstructed top quarks, while $\mathcal{O}_3$ consists of the four-momenta of the charged leptons and the b quarks originating from the top quarks. Asymmetries in these observables are sensitive to CP violation, and their measurement is used to determine the chromoelectric dipole moment of the top quark. The results are consistent with the expectation from the standard model.
Measured asymmetries of O_1 and O_3 with statistical uncertainties
The measured asymmetries of O_1 and O_3, and dimensionless CEDM \ImdtG, extracted using the asymmetries in O_1 and O_3, with their uncertainties.
Results for the covariance matrix where the parameters a and b are taken from a linear fit (equation 11) to the different CP-violating samples (CEMD).
In this paper Au+Au collisions at 11.6A GeV/c are characterized by two global observables: the energy measured near zero degrees (EZCAL) and the total event multiplicity. Particle spectra are measured for different event classes that are defined in a two-dimensional grid of both global observables. For moderately central events (σ/σint<12%) the proton dN/dy distributions do not depend on EZCAL but only on the event multiplicity. In contrast the shape of the proton transverse spectra shows little dependence on the event multiplicity. The change in the proton dN/dy distributions suggests that different conditions are formed in the collision for different event classes. These event classes are studied for signals of new physics by measuring pion and kaon spectra and yields. In the event classes doubly selected on EZCAL and multiplicity there is no indication of any unusual pion or kaon yields, spectra, or K/π ratio even in the events with extreme multiplicity.
Table for event classification (from CLASS1 to CLASS8) where ZCAL energy solely used for event selection. Number of Projectile Participants Npp=197*(1-E(P=3)/EKIN(P=1)).
CLASS1 (see Table for event classification).
CLASS1 (see Table for event classification).
CLASS1 (see Table for event classification).
CLASS2 (see Table for event classification).
CLASS2 (see Table for event classification).
CLASS2 (see Table for event classification).
CLASS3 (see Table for event classification).
CLASS3 (see Table for event classification).
CLASS3 (see Table for event classification).
Table for event classification (from CLASS1 to CLASS8) where ZCAL energy s olely used for event selection. Number of Projectile Participants Npp=197*(1-E(P=3)/EKIN(P=1)).
CLASS1 (see Table for event classification).
CLASS2 (see Table for event classification).
CLASS3 (see Table for event classification).
CLASS4 (see Table for event classification).
CLASS5 (see Table for event classification).
CLASS6 (see Table for event classification).
CLASS7 (see Table for event classification).
CLASS8 (see Table for event classification).
Table for event classification (from CLASS1 to CLASS8) where ZCAL energy s olely used for event selection. Number of Projectile Participants Npp=197*(1-E(P=3)/EKIN(P=1)).
CLASS1 (see Table for event classification).
CLASS1 (see Table for event classification).
CLASS1 (see Table for event classification).
CLASS2 (see Table for event classification).
CLASS2 (see Table for event classification).
CLASS2 (see Table for event classification).
CLASS3 (see Table for event classification).
CLASS3 (see Table for event classification).
CLASS3 (see Table for event classification).
Table for event classification (from CLASS1 to CLASS8) where ZCAL energy s olely used for event selection. Number of Projectile Participants Npp=197*(1-E(P=3)/EKIN(P=1)).
CLASS1 (see Table for event classification).
CLASS2 (see Table for event classification).
CLASS3 (see Table for event classification).
CLASS4 (see Table for event classification).
CLASS5 (see Table for event classification).
CLASS6 (see Table for event classification).
CLASS7 (see Table for event classification).
CLASS8 (see Table for event classification).
Table for event classification (from CLASS1 to CLASS8) where ZCAL energy s olely used for event selection. Number of Projectile Participants Npp=197*(1-E(P=3)/EKIN(P=1)).
CLASS1 (see Table for event classification).
CLASS1 (see Table for event classification).
CLASS1 (see Table for event classification).
CLASS2 (see Table for event classification).
CLASS2 (see Table for event classification).
CLASS2 (see Table for event classification).
CLASS3 (see Table for event classification).
CLASS3 (see Table for event classification).
CLASS3 (see Table for event classification).
This paper presents a measurement of the $W$ boson production cross section and the $W^{+}/W^{-}$ cross-section ratio, both in association with jets, in proton--proton collisions at $\sqrt{s}=8$ TeV with the ATLAS experiment at the Large Hadron Collider. The measurement is performed in final states containing one electron and missing transverse momentum using data corresponding to an integrated luminosity of 20.2 fb$^{-1}$. Differential cross sections for events with one or two jets are presented for a range of observables, including jet transverse momenta and rapidities, the scalar sum of transverse momenta of the visible particles and the missing transverse momentum in the event, and the transverse momentum of the $W$ boson. For a subset of the observables, the differential cross sections of positively and negatively charged $W$ bosons are measured separately. In the cross-section ratio of $W^{+}/W^{-}$ the dominant systematic uncertainties cancel out, improving the measurement precision by up to a factor of nine. The observables and ratios selected for this paper provide valuable input for the up quark, down quark, and gluon parton distribution functions of the proton.
Cross section for the production of W bosons for different inclusive jet multiplicities.
Statistical correlation between bins in data for the cross section for the production of W bosons for different inclusive jet multiplicities.
Differential cross sections for the production of W<sup>+</sup> bosons, W<sup>-</sup> bosons and the W<sup>+</sup>/W<sup>-</sup> cross section ratio as a function of the inclusive jet multiplicity.
Statistical correlation between bins in data for the differential cross sections for the production of W<sup>+</sup> bosons as a function of the inclusive jet multiplicity.
Statistical correlation between bins in data for the differential cross sections for the production of W<sup>-</sup> bosons as a function of the inclusive jet multiplicity.
Differential cross section for the production of W bosons as a function of H<sub> T</sub> for events with N<sub> jets</sub> ≥ 1.
Statistical correlation between bins in data for the differential cross section for the production of W bosons as a function of H<sub> T</sub> for events with N<sub> jets</sub> ≥ 1.
Differential cross sections for the production of W<sup>+</sup> bosons, W<sup>-</sup> bosons and the W<sup>+</sup>/W<sup>-</sup> cross section ratio as a function of the H<sub> T</sub> for events with N<sub> jets</sub> ≥ 1.
Statistical correlation between bins in data for the differential cross sections for the production of W<sup>+</sup> bosons as a function of the H<sub> T</sub> for events with N<sub> jets</sub> ≥ 1.
Statistical correlation between bins in data for the differential cross sections for the production of W<sup>-</sup> bosons as a function of the H<sub> T</sub> for events with N<sub> jets</sub> ≥ 1.
Differential cross section for the production of W bosons as a function of the W p<sub>T</sub> for events with N<sub> jets</sub> ≥ 1.
Statistical correlation between bins in data for the differential cross section for the production of W bosons as a function of the W p<sub>T</sub> for events with N<sub> jets</sub> ≥ 1.
Differential cross sections for the production of W<sup>+</sup> bosons, W<sup>-</sup> bosons and the W<sup>+</sup>/W<sup>-</sup> cross section ratio as a function of the W p<sub>T</sub> for events with N<sub> jets</sub> ≥ 1.
Statistical correlation between bins in data for the differential cross sections for the production of W<sup>+</sup> bosons as a function of the W p<sub>T</sub> for events with N<sub> jets</sub> ≥ 1.
Statistical correlation between bins in data for the differential cross sections for the production of W<sup>-</sup> bosons as a function of the W p<sub>T</sub> for events with N<sub> jets</sub> ≥ 1.
Differential cross section for the production of W bosons as a function of the leading jet p<sub>T</sub> for events with N<sub> jets</sub> ≥ 1.
Statistical correlation between bins in data for the differential cross section for the production of W bosons as a function of the leading jet p<sub>T</sub> for events with N<sub> jets</sub> ≥ 1.
Differential cross sections for the production of W<sup>+</sup> bosons, W<sup>-</sup> bosons and the W<sup>+</sup>/W<sup>-</sup> cross section ratio as a function of the leading jet p<sub>T</sub> for events with N<sub> jets</sub> ≥ 1.
Statistical correlation between bins in data for the differential cross sections for the production of W<sup>+</sup> bosons as a function of the leading jet p<sub>T</sub> for events with N<sub> jets</sub> ≥ 1.
Statistical correlation between bins in data for the differential cross sections for the production of W<sup>-</sup> bosons as a function of the leading jet p<sub>T</sub> for events with N<sub> jets</sub> ≥ 1.
Differential cross section for the production of W bosons as a function of the leading jet rapidity for events with N<sub> jets</sub> ≥ 1.
Statistical correlation between bins in data for the differential cross section for the production of W bosons as a function of the leading jet rapidity for events with N<sub> jets</sub> ≥ 1.
Differential cross sections for the production of W<sup>+</sup> bosons, W<sup>-</sup> bosons and the W<sup>+</sup>/W<sup>-</sup> cross section ratio as a function of the leading jet rapidity for events with N<sub> jets</sub> ≥ 1.
Statistical correlation between bins in data for the differential cross sections for the production of W<sup>+</sup> bosons as a function of the leading jet rapidity for events with N<sub> jets</sub> ≥ 1.
Statistical correlation between bins in data for the differential cross sections for the production of W<sup>-</sup> bosons as a function of the leading jet rapidity for events with N<sub> jets</sub> ≥ 1.
Differential cross section for the production of W bosons as a function of second leading jet p<sub>T</sub> for events with N<sub> jets</sub> ≥ 2.
Statistical correlation between bins in data for the differential cross section for the production of W bosons as a function of second leading jet p<sub>T</sub> for events with N<sub> jets</sub> ≥ 2.
Differential cross section for the production of W bosons as a function of second leading jet rapidity for events with N<sub> jets</sub> ≥ 2.
Statistical correlation between bins in data for the differential cross section for the production of W bosons as a function of second leading jet rapidity for events with N<sub> jets</sub> ≥ 2.
Differential cross section for the production of W bosons as a function of Δ R<sub>jet1,jet2</sub> for events with N<sub> jets</sub> ≥ 2.
Statistical correlation between bins in data for the differential cross section for the production of W bosons as a function of Δ R<sub>jet1,jet2</sub> for events with N<sub> jets</sub> ≥ 2.
Differential cross section for the production of W bosons as a function of dijet invariant mass for events with N<sub> jets</sub> ≥ 2.
Statistical correlation between bins in data for the differential cross section for the production of W bosons as a function of dijet invariant mass for events with N<sub> jets</sub> ≥ 2.
Cross section for the production of W bosons as a function of exclusive jet multiplicity.
Statistical correlation between bins in data for the cross section for the production of W bosons as a function of exclusive jet multiplicity.
Differential cross section for the production of W bosons as a function of the H<sub> T</sub> for events with N<sub> jets</sub> ≥ 2.
Statistical correlation between bins in data for the differential cross section for the production of W bosons as a function of the H<sub> T</sub> for events with N<sub> jets</sub> ≥ 2.
Differential cross sections for the production of W<sup>+</sup> bosons, W<sup>-</sup> bosons and the W<sup>+</sup>/W<sup>-</sup> cross section ratio as a function of the H<sub> T</sub> for events with N<sub> jets</sub> ≥ 2.
Statistical correlation between bins in data for the differential cross sections for the production of W<sup>+</sup> bosons as a function of the H<sub> T</sub> for events with N<sub> jets</sub> ≥ 2.
Statistical correlation between bins in data for the differential cross sections for the production of W<sup>-</sup> bosons as a function of the H<sub> T</sub> for events with N<sub> jets</sub> ≥ 2.
Differential cross section for the production of W bosons as a function of the W p<sub>T</sub> for events with N<sub> jets</sub> ≥ 2.
Statistical correlation between bins in data for the differential cross section for the production of W bosons as a function of the W p<sub>T</sub> for events with N<sub> jets</sub> ≥ 2.
Differential cross sections for the production of W<sup>+</sup> bosons, W<sup>-</sup> bosons and the W<sup>+</sup>/W<sup>-</sup> cross section ratio as a function of the W p<sub>T</sub> for events with N<sub> jets</sub> ≥ 2.
Statistical correlation between bins in data for the differential cross sections for the production of W<sup>+</sup> bosons as a function of the W p<sub>T</sub> for events with N<sub> jets</sub> ≥ 2.
Statistical correlation between bins in data for the differential cross sections for the production of W<sup>-</sup> bosons as a function of the W p<sub>T</sub> for events with N<sub> jets</sub> ≥ 2.
Differential cross section for the production of W bosons as a function of the leading jet p<sub>T</sub> for events with N<sub> jets</sub> ≥ 2.
Statistical correlation between bins in data for the differential cross section for the production of W bosons as a function of the leading jet p<sub>T</sub> for events with N<sub> jets</sub> ≥ 2.
Differential cross sections for the production of W<sup>+</sup> bosons, W<sup>-</sup> bosons and the W<sup>+</sup>/W<sup>-</sup> cross section ratio as a function of the leading jet p<sub>T</sub> for events with N<sub> jets</sub> ≥ 2.
Statistical correlation between bins in data for the differential cross sections for the production of W<sup>+</sup> bosons as a function of the leading jet p<sub>T</sub> for events with N<sub> jets</sub> ≥ 2.
Statistical correlation between bins in data for the differential cross sections for the production of W<sup>-</sup> bosons as a function of the leading jet p<sub>T</sub> for events with N<sub> jets</sub> ≥ 2.
Differential cross section for the production of W bosons as a function of the electron η for events with N<sub> jets</sub> ≥ 0.
Statistical correlation between bins in data for the differential cross section for the production of W bosons as a function of the electron η for events with N<sub> jets</sub> ≥ 0.
Differential cross sections for the production of W<sup>+</sup> bosons, W<sup>-</sup> bosons and the W<sup>+</sup>/W<sup>-</sup> cross section ratio as a function of the electron η for events with N<sub> jets</sub> ≥ 0.
Statistical correlation between bins in data for the differential cross sections for the production of W<sup>+</sup> bosons as a function of the electron η for events with N<sub> jets</sub> ≥ 0.
Statistical correlation between bins in data for the differential cross sections for the production of W<sup>-</sup> bosons as a function of the electron η for events with N<sub> jets</sub> ≥ 0.
Differential cross section for the production of W bosons as a function of the electron η for events with N<sub> jets</sub> ≥ 1.
Statistical correlation between bins in data for the differential cross section for the production of W bosons as a function of the electron η for events with N<sub> jets</sub> ≥ 1.
Differential cross sections for the production of W<sup>+</sup> bosons, W<sup>-</sup> bosons and the W<sup>+</sup>/W<sup>-</sup> cross section ratio as a function of the electron η for events with N<sub> jets</sub> ≥ 1.
Statistical correlation between bins in data for the differential cross sections for the production of W<sup>+</sup> bosons as a function of the electron η for events with N<sub> jets</sub> ≥ 1.
Statistical correlation between bins in data for the differential cross sections for the production of W<sup>-</sup> bosons as a function of the electron η for events with N<sub> jets</sub> ≥ 1.
List of experimentally considered systematic uncertainties for the W+jets cross section measurement
Non-perturbative corrections for the cross section for the production of W bosons for different inclusive jet multiplicities.
Non-perturbative corrections for the differential cross sections for the production of W<sup>+</sup> bosons and W<sup>-</sup> bosons as a function of the inclusive jet multiplicity.
Non-perturbative corrections for the differential cross section for the production of W bosons as a function of H<sub> T</sub> for events with N<sub> jets</sub> ≥ 1.
Non-perturbative corrections for the differential cross sections for the production of W<sup>+</sup> bosons and W<sup>-</sup> bosons as a function of the H<sub> T</sub> for events with N<sub> jets</sub> ≥ 1.
Non-perturbative corrections for the differential cross section for the production of W bosons as a function of the W p<sub>T</sub> for events with N<sub> jets</sub> ≥ 1.
Non-perturbative corrections for the differential cross sections for the production of W<sup>+</sup> bosons and W<sup>-</sup> bosons as a function of the W p<sub>T</sub> for events with N<sub> jets</sub> ≥ 1.
Non-perturbative corrections for the differential cross section for the production of W bosons as a function of the leading jet p<sub>T</sub> for events with N<sub> jets</sub> ≥ 1.
Non-perturbative corrections for the differential cross sections for the production of W<sup>+</sup> bosons and W<sup>-</sup> bosons as a function of the leading jet p<sub>T</sub> for events with N<sub> jets</sub> ≥ 1.
Non-perturbative corrections for the differential cross section for the production of W bosons as a function of the leading jet rapidity for events with N<sub> jets</sub> ≥ 1.
Non-perturbative corrections for the differential cross sections for the production of W<sup>+</sup> bosons and W<sup>-</sup> bosons as a function of the leading jet rapidity for events with N<sub> jets</sub> ≥ 1.
Non-perturbative corrections for the differential cross section for the production of W bosons as a function of second leading jet p<sub>T</sub> for events with N<sub> jets</sub> ≥ 2.
Non-perturbative corrections for the differential cross section for the production of W bosons as a function of second leading jet rapidity for events with N<sub> jets</sub> ≥ 2.
Non-perturbative corrections for the differential cross section for the production of W bosons as a function of Δ R<sub>jet1,jet2</sub> for events with N<sub> jets</sub> ≥ 2.
Non-perturbative corrections for the differential cross section for the production of W bosons as a function of dijet invariant mass for events with N<sub> jets</sub> ≥ 2.
Non-perturbative corrections for the cross section for the production of W bosons as a function of exclusive jet multiplicity.
Non-perturbative corrections for the differential cross section for the production of W bosons as a function of the H<sub> T</sub> for events with N<sub> jets</sub> ≥ 2.
Non-perturbative corrections for the differential cross sections for the production of W<sup>+</sup> bosons and W<sup>-</sup> bosons as a function of the H<sub> T</sub> for events with N<sub> jets</sub> ≥ 2.
Non-perturbative corrections for the differential cross section for the production of W bosons as a function of the W p<sub>T</sub> for events with N<sub> jets</sub> ≥ 2.
Non-perturbative corrections for the differential cross sections for the production of W<sup>+</sup> bosons and W<sup>-</sup> bosons as a function of the W p<sub>T</sub> for events with N<sub> jets</sub> ≥ 2.
Non-perturbative corrections for the differential cross section for the production of W bosons as a function of the leading jet p<sub>T</sub> for events with N<sub> jets</sub> ≥ 2.
Non-perturbative corrections for the differential cross sections for the production of W<sup>+</sup> bosons and W<sup>-</sup> bosons as a function of the leading jet p<sub>T</sub> for events with N<sub> jets</sub> ≥ 2.
NNLO/NLO k-factors determined with NNLO Njetti for the differential cross sections for the production of W<sup>+</sup> bosons and W<sup>-</sup> bosons as a function of the H<sub> T</sub> for events with N<sub> jets</sub> ≥ 1. These numbers were obtained with code described in Phys. Rev. Lett. 115 (2015) 062002 [arXiv:1504.02131].
NNLO/NLO k-factors determined with NNLO Njetti for the differential cross sections for the production of W<sup>+</sup> bosons and W<sup>-</sup> bosons as a function of the W p<sub>T</sub> for events with N<sub> jets</sub> ≥ 1. These numbers were obtained with code described in Phys. Rev. Lett. 115 (2015) 062002 [arXiv:1504.02131].
NNLO/NLO k-factors determined with NNLO Njetti for the differential cross sections for the production of W<sup>+</sup> bosons and W<sup>-</sup> bosons as a function of the leading jet p<sub>T</sub> for events with N<sub> jets</sub> ≥ 1. These numbers were obtained with code described in Phys. Rev. Lett. 115 (2015) 062002 [arXiv:1504.02131].
NNLO/NLO k-factors determined with NNLO Njetti for the differential cross sections for the production of W<sup>+</sup> bosons and W<sup>-</sup> bosons as a function of the leading jet rapidity for events with N<sub> jets</sub> ≥ 1. These numbers were obtained with code described in Phys. Rev. Lett. 115 (2015) 062002 [arXiv:1504.02131].
Spin transfer from circularly polarized real photons to recoiling hyperons has been measured for the reactions $\vec\gamma + p \to K^+ + \vec\Lambda$ and $\vec\gamma + p \to K^+ + \vec\Sigma^0$. The data were obtained using the CLAS detector at Jefferson Lab for center-of-mass energies $W$ between 1.6 and 2.53 GeV, and for $-0.85<\cos\theta_{K^+}^{c.m.}< +0.95$. For the $\Lambda$, the polarization transfer coefficient along the photon momentum axis, $C_z$, was found to be near unity for a wide range of energy and kaon production angles. The associated transverse polarization coefficient, $C_x$, is smaller than $C_z$ by a roughly constant difference of unity. Most significantly, the {\it total} $\Lambda$ polarization vector, including the induced polarization $P$, has magnitude consistent with unity at all measured energies and production angles when the beam is fully polarized. For the $\Sigma^0$ this simple phenomenology does not hold. All existing hadrodynamic models are in poor agreement with these results.
Coefficients Cx and Cz for the reaction GAMMA P --> K+ LAMBDA for incident energy = 1.032 GeV and W = 1.679 GeV.
Coefficients Cx and Cz for the reaction GAMMA P --> K+ LAMBDA for incident energy = 1.132 GeV and W = 1.734 GeV.
Coefficients Cx and Cz for the reaction GAMMA P --> K+ LAMBDA for incident energy = 1.232 GeV and W = 1.787 GeV.
Coefficients Cx and Cz for the reaction GAMMA P --> K+ LAMBDA for incident energy = 1.332 GeV and W = 1.839 GeV.
Coefficients Cx and Cz for the reaction GAMMA P --> K+ LAMBDA for incident energy = 1.433 GeV and W = 1.889 GeV.
Coefficients Cx and Cz for the reaction GAMMA P --> K+ LAMBDA for incident energy = 1.534 GeV and W = 1.939 GeV.
Coefficients Cx and Cz for the reaction GAMMA P --> K+ LAMBDA for incident energy = 1.635 GeV and W = 1.987 GeV.
Coefficients Cx and Cz for the reaction GAMMA P --> K+ LAMBDA for incident energy = 1.737 GeV and W = 2.035 GeV.
Coefficients Cx and Cz for the reaction GAMMA P --> K+ LAMBDA for incident energy = 1.838 GeV and W = 2.081 GeV.
Coefficients Cx and Cz for the reaction GAMMA P --> K+ LAMBDA for incident energy = 1.939 GeV and W = 2.126 GeV.
Coefficients Cx and Cz for the reaction GAMMA P --> K+ LAMBDA for incident energy = 2.039 GeV and W = 2.170 GeV.
Coefficients Cx and Cz for the reaction GAMMA P --> K+ LAMBDA for incident energy = 2.139 GeV and W = 2.212 GeV.
Coefficients Cx and Cz for the reaction GAMMA P --> K+ LAMBDA for incident energy = 2.240 GeV and W = 2.255 GeV.
Coefficients Cx and Cz for the reaction GAMMA P --> K+ LAMBDA for incident energy = 2.341 GeV and W = 2.296 GeV.
Coefficients Cx and Cz for the reaction GAMMA P --> K+ LAMBDA for incident energy = 2.443 GeV and W = 2.338 GeV.
Coefficients Cx and Cz for the reaction GAMMA P --> K+ LAMBDA for incident energy = 2.543 GeV and W = 2.377 GeV.
Coefficients Cx and Cz for the reaction GAMMA P --> K+ LAMBDA for incident energy = 2.642 GeV and W = 2.416 GeV.
Coefficients Cx and Cz for the reaction GAMMA P --> K+ LAMBDA for incident energy = 2.741 GeV and W = 2.454 GeV.
Coefficients Cx and Cz for the reaction GAMMA P --> K+ SIGMA0 for incident energy = 1.232 GeV and W = 1.787 GeV.
Coefficients Cx and Cz for the reaction GAMMA P --> K+ SIGMA0 for incident energy = 1.332 GeV and W = 1.839 GeV.
Coefficients Cx and Cz for the reaction GAMMA P --> K+ SIGMA0 for incident energy = 1.433 GeV and W = 1.889 GeV.
Coefficients Cx and Cz for the reaction GAMMA P --> K+ SIGMA0 for incident energy = 1.534 GeV and W = 1.939 GeV.
Coefficients Cx and Cz for the reaction GAMMA P --> K+ SIGMA0 for incident energy = 1.635 GeV and W = 1.987 GeV.
Coefficients Cx and Cz for the reaction GAMMA P --> K+ SIGMA0 for incident energy = 1.737 GeV and W = 2.035 GeV.
Coefficients Cx and Cz for the reaction GAMMA P --> K+ SIGMA0 for incident energy = 1.838 GeV and W = 2.081 GeV.
Coefficients Cx and Cz for the reaction GAMMA P --> K+ SIGMA0 for incident energy = 1.939 GeV and W = 2.126 GeV.
Coefficients Cx and Cz for the reaction GAMMA P --> K+ SIGMA0 for incident energy = 2.039 GeV and W = 2.170 GeV.
Coefficients Cx and Cz for the reaction GAMMA P --> K+ SIGMA0 for incident energy = 2.139 GeV and W = 2.212 GeV.
Coefficients Cx and Cz for the reaction GAMMA P --> K+ SIGMA0 for incident energy = 2.240 GeV and W = 2.255 GeV.
Coefficients Cx and Cz for the reaction GAMMA P --> K+ SIGMA0 for incident energy = 2.341 GeV and W = 2.296 GeV.
Coefficients Cx and Cz for the reaction GAMMA P --> K+ SIGMA0 for incident energy = 2.443 GeV and W = 2.338 GeV.
Coefficients Cx and Cz for the reaction GAMMA P --> K+ SIGMA0 for incident energy = 2.543 GeV and W = 2.377 GeV.
Coefficients Cx and Cz for the reaction GAMMA P --> K+ SIGMA0 for incident energy = 2.642 GeV and W = 2.416 GeV.
Coefficients Cx and Cz for the reaction GAMMA P --> K+ SIGMA0 for incident energy = 2.741 GeV and W = 2.454 GeV.
A measurement of jet substructure observables is presented using \ttbar events in the lepton+jets channel from proton-proton collisions at $\sqrt{s}=$ 13 TeV recorded by the CMS experiment at the LHC, corresponding to an integrated luminosity of 35.9 fb$^{-1}$. Multiple jet substructure observables are measured for jets identified as bottom, light-quark, and gluon jets, as well as for inclusive jets (no flavor information). The results are unfolded to the particle level and compared to next-to-leading-order predictions from POWHEG interfaced with the parton shower generators PYTHIA 8 and HERWIG 7, as well as from SHERPA 2 and DIRE2. A value of the strong coupling at the Z boson mass, $\alpha_S(m_\mathrm{Z}) = $ 0.115$^{+0.015}_{-0.013}$, is extracted from the substructure data at leading-order plus leading-log accuracy.
Distribution of $\lambda_{0}^{0}$ (N) reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $\lambda_{0}^{0}$ (N) reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $\lambda_{0}^{2}$ ($p_{T}^{d,*})$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $\lambda_{0}^{2}$ ($p_{T}^{d,*})$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $\lambda_{0.5}^{1}$ (LHA) reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $\lambda_{0.5}^{1}$ (LHA) reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $\lambda_{1}^{1}$ (width) reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $\lambda_{1}^{1}$ (width) reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $\lambda_{2}^{1}$ (thrust) reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $\lambda_{2}^{1}$ (thrust) reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $\varepsilon$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $\varepsilon$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $z_{g}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $z_{g}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $\Delta R_{g}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $\Delta R_{g}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $n_{SD}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $n_{SD}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $\tau_{21}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $\tau_{21}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $\tau_{32}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $\tau_{32}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $\tau_{43}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $\tau_{43}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $C_{1}^{(0.0)}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $C_{1}^{(0.0)}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $C_{1}^{(0.2)}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $C_{1}^{(0.2)}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $C_{1}^{(0.5)}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $C_{1}^{(0.5)}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $C_{1}^{(1.0)}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $C_{1}^{(1.0)}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $C_{1}^{(2.0)}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $C_{1}^{(2.0)}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $C_{2}^{(0.0)}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $C_{2}^{(0.0)}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $C_{2}^{(0.2)}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $C_{2}^{(0.2)}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $C_{2}^{(0.5)}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $C_{2}^{(0.5)}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $C_{2}^{(1.0)}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $C_{2}^{(1.0)}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $C_{2}^{(2.0)}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $C_{2}^{(2.0)}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $C_{3}^{(0.0)}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $C_{3}^{(0.0)}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $C_{3}^{(0.2)}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $C_{3}^{(0.2)}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $C_{3}^{(0.5)}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $C_{3}^{(0.5)}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $C_{3}^{(1.0)}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $C_{3}^{(1.0)}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $C_{3}^{(2.0)}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $C_{3}^{(2.0)}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $M_{2}^{(1)}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $M_{2}^{(1)}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $N_{2}^{(1)}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $N_{2}^{(1)}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $N_{3}^{(1)}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $N_{3}^{(1)}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $M_{2}^{(2)}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $M_{2}^{(2)}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $N_{2}^{(2)}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $N_{2}^{(2)}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $N_{3}^{(2)}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $N_{3}^{(2)}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $\lambda_{0}^{0}$ (N) reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $\lambda_{0}^{0}$ (N) reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $\lambda_{0}^{2}$ ($p_{T}^{d,*})$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $\lambda_{0}^{2}$ ($p_{T}^{d,*})$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $\lambda_{0.5}^{1}$ (LHA) reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $\lambda_{0.5}^{1}$ (LHA) reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $\lambda_{1}^{1}$ (width) reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $\lambda_{1}^{1}$ (width) reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $\lambda_{2}^{1}$ (thrust) reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $\lambda_{2}^{1}$ (thrust) reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $\varepsilon$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $\varepsilon$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $z_{g}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $z_{g}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $\Delta R_{g}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $\Delta R_{g}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $n_{SD}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $n_{SD}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $\tau_{21}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $\tau_{21}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $\tau_{32}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $\tau_{32}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $\tau_{43}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $\tau_{43}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $C_{1}^{(0.0)}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $C_{1}^{(0.0)}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $C_{1}^{(0.2)}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $C_{1}^{(0.2)}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $C_{1}^{(0.5)}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $C_{1}^{(0.5)}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $C_{1}^{(1.0)}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $C_{1}^{(1.0)}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $C_{1}^{(2.0)}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $C_{1}^{(2.0)}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $C_{2}^{(0.0)}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $C_{2}^{(0.0)}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $C_{2}^{(0.2)}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $C_{2}^{(0.2)}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $C_{2}^{(0.5)}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $C_{2}^{(0.5)}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $C_{2}^{(1.0)}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $C_{2}^{(1.0)}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $C_{2}^{(2.0)}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $C_{2}^{(2.0)}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $C_{3}^{(0.0)}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $C_{3}^{(0.0)}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $C_{3}^{(0.2)}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $C_{3}^{(0.2)}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $C_{3}^{(0.5)}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $C_{3}^{(0.5)}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $C_{3}^{(1.0)}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $C_{3}^{(1.0)}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $C_{3}^{(2.0)}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $C_{3}^{(2.0)}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $M_{2}^{(1)}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $M_{2}^{(1)}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $N_{2}^{(1)}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $N_{2}^{(1)}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $N_{3}^{(1)}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $N_{3}^{(1)}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $M_{2}^{(2)}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $M_{2}^{(2)}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $N_{2}^{(2)}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $N_{2}^{(2)}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $N_{3}^{(2)}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Distribution of $N_{3}^{(2)}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $\lambda_{0}^{0}$ (N) reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $\lambda_{0}^{0}$ (N) reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $\lambda_{0}^{2}$ ($p_{T}^{d,*})$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $\lambda_{0}^{2}$ ($p_{T}^{d,*})$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $\lambda_{0.5}^{1}$ (LHA) reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $\lambda_{0.5}^{1}$ (LHA) reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $\lambda_{1}^{1}$ (width) reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $\lambda_{1}^{1}$ (width) reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $\lambda_{2}^{1}$ (thrust) reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $\lambda_{2}^{1}$ (thrust) reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $\varepsilon$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $\varepsilon$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $z_{g}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $z_{g}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $\Delta R_{g}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $\Delta R_{g}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $n_{SD}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $n_{SD}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $\tau_{21}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $\tau_{21}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $\tau_{32}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $\tau_{32}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $\tau_{43}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $\tau_{43}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $C_{1}^{(0.0)}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $C_{1}^{(0.0)}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $C_{1}^{(0.2)}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $C_{1}^{(0.2)}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $C_{1}^{(0.5)}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $C_{1}^{(0.5)}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $C_{1}^{(1.0)}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $C_{1}^{(1.0)}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $C_{1}^{(2.0)}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $C_{1}^{(2.0)}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $C_{2}^{(0.0)}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $C_{2}^{(0.0)}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $C_{2}^{(0.2)}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $C_{2}^{(0.2)}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $C_{2}^{(0.5)}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $C_{2}^{(0.5)}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $C_{2}^{(1.0)}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $C_{2}^{(1.0)}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $C_{2}^{(2.0)}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $C_{2}^{(2.0)}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $C_{3}^{(0.0)}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $C_{3}^{(0.0)}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $C_{3}^{(0.2)}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $C_{3}^{(0.2)}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $C_{3}^{(0.5)}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $C_{3}^{(0.5)}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $C_{3}^{(1.0)}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $C_{3}^{(1.0)}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $C_{3}^{(2.0)}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $C_{3}^{(2.0)}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $M_{2}^{(1)}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $M_{2}^{(1)}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $N_{2}^{(1)}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $N_{2}^{(1)}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $N_{3}^{(1)}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $N_{3}^{(1)}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $M_{2}^{(2)}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $M_{2}^{(2)}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $N_{2}^{(2)}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $N_{2}^{(2)}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $N_{3}^{(2)}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $N_{3}^{(2)}$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $\lambda_{0}^{0}$ (N) reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $\lambda_{0}^{0}$ (N) reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $\lambda_{0}^{2}$ ($p_{T}^{d,*})$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $\lambda_{0}^{2}$ ($p_{T}^{d,*})$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $\lambda_{0.5}^{1}$ (LHA) reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $\lambda_{0.5}^{1}$ (LHA) reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $\lambda_{1}^{1}$ (width) reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $\lambda_{1}^{1}$ (width) reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $\lambda_{2}^{1}$ (thrust) reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $\lambda_{2}^{1}$ (thrust) reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $\varepsilon$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $\varepsilon$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $z_{g}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $z_{g}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $\Delta R_{g}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $\Delta R_{g}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $n_{SD}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $n_{SD}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $\tau_{21}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $\tau_{21}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $\tau_{32}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $\tau_{32}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $\tau_{43}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $\tau_{43}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $C_{1}^{(0.0)}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $C_{1}^{(0.0)}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $C_{1}^{(0.2)}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $C_{1}^{(0.2)}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $C_{1}^{(0.5)}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $C_{1}^{(0.5)}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $C_{1}^{(1.0)}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $C_{1}^{(1.0)}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $C_{1}^{(2.0)}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $C_{1}^{(2.0)}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $C_{2}^{(0.0)}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $C_{2}^{(0.0)}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $C_{2}^{(0.2)}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $C_{2}^{(0.2)}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $C_{2}^{(0.5)}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $C_{2}^{(0.5)}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $C_{2}^{(1.0)}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $C_{2}^{(1.0)}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $C_{2}^{(2.0)}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $C_{2}^{(2.0)}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $C_{3}^{(0.0)}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $C_{3}^{(0.0)}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $C_{3}^{(0.2)}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $C_{3}^{(0.2)}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $C_{3}^{(0.5)}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $C_{3}^{(0.5)}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $C_{3}^{(1.0)}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $C_{3}^{(1.0)}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $C_{3}^{(2.0)}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $C_{3}^{(2.0)}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $M_{2}^{(1)}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $M_{2}^{(1)}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $N_{2}^{(1)}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $N_{2}^{(1)}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $N_{3}^{(1)}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $N_{3}^{(1)}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $M_{2}^{(2)}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $M_{2}^{(2)}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $N_{2}^{(2)}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $N_{2}^{(2)}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $N_{3}^{(2)}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Covariance matrix for $N_{3}^{(2)}$ reconstructed from all particles with pt > 1 GeV, unfolded to the particle level.
Toward the goal of experimentally determining the p-p elastic-scattering amplitudes at 6 GeV/c, we have measured a number of triple- and double-spin correlation parameters over the ‖t‖ range between 0.2 and 1.0 (GeV/c)2. These new data permit the first nucleon-nucleon amplitude determination in the multi-GeV energy range. Polarized beams from the Argonne Zero Gradient Synchrotron and polarized targets were utilized. The polarization of the recoil proton was measured with a carbon polarimeter. A total of 14 different spin observables were measured (five spin transfer, four depolarization, and five triple-spin correlation parameters). These have been combined with earlier results, resulting in a data set of typically 30 measurements of 20 different spin observables for each of six ‖t‖ values between 0.2 and 1.0 (GeV/c)2. A solution for the amplitudes has been found at each ‖t‖, and comparisons are presented with several different models. The spin-nonflip helicity amplitudes are found to be much larger than the spin-flip amplitudes.
No description provided.
No description provided.
We present data of several rescattering observables measured inn p elastic scattering between 0.80 and 1.10 GeV. The SATURNE II polarized beam of free neutrons obtained from the break-up of polarized deuterons was scattered on the Saclay polarized frozen-spin proton target. Three different configurations of beam and target polarization directions were used: the observablesDonon andKonno were measured with the normal-normal spin configuration at eight energies;Nonkk,Dos″ok andKos″ko were determined with the longitudinal-longitudinal configuration at six energies;Nonsk,Dos″ok andKos″so with the sideway-longitudinal configuration at six energies. Part of the data was obtained with an unpolarized CH2 target where only the two spin-index polarization transfer parametersKos″ko andKos″so were determined. Data are compared with phase shift analyses predictions and with the LAMPF results at 0.788 GeV. Present results are the first measurements of rescattering observables above 0.80 GeV. They provide an important contribution to any future theoretical or phenomenological analysis.
No description provided.
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A new high precision measurement of the reaction pp -> pK+Lambda at a beam momentum of 2.95 GeV/c with more than 200,000 analyzed events allows a detailed analysis of differential observables and their inter-dependencies. Correlations of the angular distributions with momenta are examined. The invariant mass distributions are compared for different regions in the Dalitz plots. The cusp structure at the N Sigma threshold is described with the Flatt\'e formalism and its variation in the Dalitz plot is analyzed.
No description provided.
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deviation from phase space in arb. units.
The quasifree $\overrightarrow{\gamma} d\to\pi^0n(p)$ photon beam asymmetry, $\Sigma$, has been measured at photon energies, $E_\gamma$, from 390 to 610 MeV, corresponding to center of mass energy from 1.271 to 1.424 GeV, for the first time. The data were collected in the A2 hall of the MAMI electron beam facility with the Crystal Ball and TAPS calorimeters covering pion center-of-mass angles from 49 to 148$^\circ$. In this kinematic region, polarization observables are sensitive to contributions from the $\Delta (1232)$ and $N(1440)$ resonances. The extracted values of $\Sigma$ have been compared to predictions based on partial-wave analyses (PWAs) of the existing pion photoproduction database. Our comparison includes the SAID, MAID, and Bonn-Gatchina analyses; while a revised SAID fit, including the new $\Sigma$ measurements, has also been performed. In addition, isospin symmetry is examined as a way to predict $\pi^0n$ photoproduction observables, based on fits to published data in the channels $\pi^0p$, $\pi^+n$, and $\pi^-p$.
Photon beam asymmetry Sigma at W= 1.2711 GeV
Photon beam asymmetry Sigma at W= 1.2858 GeV
Photon beam asymmetry Sigma at W= 1.3003 GeV
Photon beam asymmetry Sigma at W= 1.3147 GeV
Photon beam asymmetry Sigma at W= 1.3289 GeV
Photon beam asymmetry Sigma at W= 1.3430 GeV
Photon beam asymmetry Sigma at W= 1.3569 GeV
Photon beam asymmetry Sigma at W= 1.3707 GeV
Photon beam asymmetry Sigma at W= 1.3843 GeV
Photon beam asymmetry Sigma at W= 1.3978 GeV
Photon beam asymmetry Sigma at W= 1.4112 GeV
Photon beam asymmetry Sigma at W= 1.4244 GeV
The strong coupling alpha_s(M_Z^2) has been measured using hadronic decays of Z^0 bosons collected by the SLD experiment at SLAC. The data were compared with QCD predictions both at fixed order, O(alpha_s^2), and including resummed analytic formulae based on the next-to-leading logarithm approximation. In this comprehensive analysis we studied event shapes, jet rates, particle correlations, and angular energy flow, and checked the consistency between alpha_s(M_Z^2) values extracted from these different measures. Combining all results we obtain alpha_s(M_Z^2) = 0.1200 \pm 0.0025(exp.) \pm 0.0078(theor.), where the dominant uncertainty is from uncalculated higher order contributions.
Final average value of alpha_s. The second (DSYS) error is from the uncertainty on the theoretical part of the calculation.
TAU is 1-THRUST.
RHO is the normalized heavy jet mass MH**2/EVIS**2.
No description provided.
No description provided.
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D2 is the differential two-jet rate here as a function of ycut, the jet algorithm cut-off parameter.. Calculated in the E scheme.
D2 is the differential two-jet rate here as a function of ycut, the jet algorithm cut-off parameter.. Calculated in the E0 scheme.
D2 is the differential two-jet rate here as a function of ycut, the jet algorithm cut-off parameter.. Calculated in the P scheme.
D2 is the differential two-jet rate here as a function of ycut, the jet algorithm cut-off parameter.. Calculated in the P0 scheme.
D2 is the differential two-jet rate here as a function of ycut, the jet algorithm cut-off parameter.. Calculated in the D scheme.
D2 is the differential two-jet rate here as a function of ycut, the jet algorithm cut-off parameter.. Calculated in the G scheme.
No description provided.
No description provided.
JCEF is the jet cone energy fraction.
Jet substructure observables have significantly extended the search program for physics beyond the Standard Model at the Large Hadron Collider. The state-of-the-art tools have been motivated by theoretical calculations, but there has never been a direct comparison between data and calculations of jet substructure observables that are accurate beyond leading-logarithm approximation. Such observables are significant not only for probing the collinear regime of QCD that is largely unexplored at a hadron collider, but also for improving the understanding of jet substructure properties that are used in many studies at the Large Hadron Collider. This Letter documents a measurement of the first jet substructure quantity at a hadron collider to be calculated at next-to-next-to-leading-logarithm accuracy. The normalized, differential cross-section is measured as a function of log$_{10}\rho^2$, where $\rho$ is the ratio of the soft-drop mass to the ungroomed jet transverse momentum. This quantity is measured in dijet events from 32.9 fb$^{-1}$ of $\sqrt{s} = 13$ TeV proton-proton collisions recorded by the ATLAS detector. The data are unfolded to correct for detector effects and compared to precise QCD calculations and leading-logarithm particle-level Monte Carlo simulations.
Data from Fig 3a. The unfolded $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with $p_T$(lead) > 600 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data; the uncertainties from the calculations are shown on each one. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from Fig 3a. The unfolded $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with $p_T$(lead) > 600 GeV, after the soft drop algorithm is applied for $\beta$ = 0, in data. All uncertainties described in the text are shown on the data; the uncertainties from the calculations are shown on each one. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from Fig 3b. The unfolded $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with $p_T$(lead) > 600 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data; the uncertainties from the calculations are shown on each one. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from Fig 3b. The unfolded $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with $p_T$(lead) > 600 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data; the uncertainties from the calculations are shown on each one. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from Fig 3c. The unfolded $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with $p_T$(lead) > 600 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data; the uncertainties from the calculations are shown on each one. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$. The uncertainties are applied symmetrically, though the cross section cannot go below zero in the first bin.
Data from Fig 3c. The unfolded $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with $p_T$(lead) > 600 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data; the uncertainties from the calculations are shown on each one. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$. The uncertainties are applied symmetrically, though the cross section cannot go below zero in the first bin.
Data from Fig 4 and Fig 8a-16a. The unfolded $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with $p_T$(lead) > 600 GeV, after the soft drop algorithm is applied for beta = 0, in data. All uncertainties described in the text are shown on the data; the uncertainties from the calculations are shown on each one. The distributions are normalized to the integrated cross section, sigma(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$. Each set of 10 bins corresponds to one $p_T$ bin in {600, 650, 700, 750, 800, 850, 900, 950, 1000, ∞ } and 10 evenly spaced bins in $log_{10}(\rho^2)$ from -4.5 to -0.5.
Data from FigAux 4 and FigAux 8a-16a. The unfolded $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with $p_T$(lead) > 600 GeV, after the soft drop algorithm is applied for beta = 0, in data. All uncertainties described in the text are shown on the data; the uncertainties from the calculations are shown on each one. The distributions are normalized to the integrated cross section, sigma(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$. Each set of 10 bins corresponds to one $p_T$ bin in {600, 650, 700, 750, 800, 850, 900, 950, 1000, ∞ } and 10 evenly spaced bins in $log_{10}(\rho^2)$ from -4.5 to -0.5.
Data from Fig 4 and Fig 8b-16b. The unfolded $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with $p_T$(lead) > 600 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data; the uncertainties from the calculations are shown on each one. The distributions are normalized to the integrated cross section, sigma(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$. Each set of 10 bins corresponds to one $p_T$ bin in {600, 650, 700, 750, 800, 850, 900, 950, 1000, ∞ } and 10 evenly spaced bins in $log_{10}(\rho^2)$ from -4.5 to -0.5.
Data from FigAux 4 and FigAux 8b-16b. The unfolded $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with $p_T$(lead) > 600 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data; the uncertainties from the calculations are shown on each one. The distributions are normalized to the integrated cross section, sigma(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$. Each set of 10 bins corresponds to one $p_T$ bin in {600, 650, 700, 750, 800, 850, 900, 950, 1000, ∞ } and 10 evenly spaced bins in $log_{10}(\rho^2)$ from -4.5 to -0.5.
Data from Fig 8c-16c. The unfolded $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with $p_T$(lead) > 600 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data; the uncertainties from the calculations are shown on each one. The distributions are normalized to the integrated cross section, sigma(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$. Each set of 10 bins corresponds to one $p_T$ bin in {600, 650, 700, 750, 800, 850, 900, 950, 1000, ∞ } and 10 evenly spaced bins in $log_{10}(\rho^2)$ from -4.5 to -0.5.
Data from FigAux 8c-16c. The unfolded $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with $p_T$(lead) > 600 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data; the uncertainties from the calculations are shown on each one. The distributions are normalized to the integrated cross section, sigma(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$. Each set of 10 bins corresponds to one $p_T$ bin in {600, 650, 700, 750, 800, 850, 900, 950, 1000, ∞ } and 10 evenly spaced bins in $log_{10}(\rho^2)$ from -4.5 to -0.5.
Data from Fig 6a. The summed covariance matrices of the systematic and statistical uncertainties for the combined $p_T$ and $log_{10}(\rho^2)$ bins for $\beta$ = 0. Each group of 10 bins corresponds to a bin of $p_T$ in {600, 650, 700, 750, 800, 850, 900, 950, 1000, ∞ }; each bin within the $p_T$ bin corresponds to 10 evenly spaced bins in $log_{10}(\rho^2)$ from -4.5 to -0.5.
Data from FigAux 6a. The summed covariance matrices of the systematic and statistical uncertainties for the combined $p_T$ and $log_{10}(\rho^2)$ bins for $\beta$ = 0. Each group of 10 bins corresponds to a bin of $p_T$ in {600, 650, 700, 750, 800, 850, 900, 950, 1000, ∞ }; each bin within the $p_T$ bin corresponds to 10 evenly spaced bins in $log_{10}(\rho^2)$ from -4.5 to -0.5.
Data from Fig 6b. The summed covariance matrices of the systematic and statistical uncertainties for the combined $p_T$ and $log_{10}(\rho^2)$ bins for $\beta$ = 1. Each group of 10 bins corresponds to a bin of $p_T$ in {600, 650, 700, 750, 800, 850, 900, 950, 1000, ∞ }; each bin within the $p_T$ bin corresponds to 10 evenly spaced bins in $log_{10}(\rho^2)$ from -4.5 to -0.5.
Data from FigAux 6b. The summed covariance matrices of the systematic and statistical uncertainties for the combined $p_T$ and $log_{10}(\rho^2)$ bins for $\beta$ = 1. Each group of 10 bins corresponds to a bin of $p_T$ in {600, 650, 700, 750, 800, 850, 900, 950, 1000, ∞ }; each bin within the $p_T$ bin corresponds to 10 evenly spaced bins in $log_{10}(\rho^2)$ from -4.5 to -0.5.
Data from Fig 6c. The summed covariance matrices of the systematic and statistical uncertainties for the combined $p_T$ and $log_{10}(\rho^2)$ bins for $\beta$ = 2. Each group of 10 bins corresponds to a bin of $p_T$ in {600, 650, 700, 750, 800, 850, 900, 950, 1000, ∞ }; each bin within the $p_T$ bin corresponds to 10 evenly spaced bins in $log_{10}(\rho^2)$ from -4.5 to -0.5.
Data from FigAux 6c. The summed covariance matrices of the systematic and statistical uncertainties for the combined $p_T$ and $log_{10}(\rho^2)$ bins for $\beta$ = 2. Each group of 10 bins corresponds to a bin of $p_T$ in {600, 650, 700, 750, 800, 850, 900, 950, 1000, ∞ }; each bin within the $p_T$ bin corresponds to 10 evenly spaced bins in $log_{10}(\rho^2)$ from -4.5 to -0.5.
Data from Fig 7a. The summed covariance matrices of the systematic and statistical uncertainties for the $log_{10}(\rho^2)$ bins for $\beta$ = 0, inclusive in $p_T$.
Data from FigAux 7a. The summed covariance matrices of the systematic and statistical uncertainties for the $log_{10}(\rho^2)$ bins for $\beta$ = 0, inclusive in $p_T$.
Data from Fig 7b. The summed covariance matrices of the systematic and statistical uncertainties for the $log_{10}(\rho^2)$ bins for $\beta$ = 1, inclusive in $p_T$.
Data from FigAux 7b. The summed covariance matrices of the systematic and statistical uncertainties for the $log_{10}(\rho^2)$ bins for $\beta$ = 1, inclusive in $p_T$.
Data from Fig 7c. The summed covariance matrices of the systematic and statistical uncertainties for the $log_{10}(\rho^2)$ bins for $\beta$ = 2, inclusive in $p_T$.
Data from FigAux 7c. The summed covariance matrices of the systematic and statistical uncertainties for the $log_{10}(\rho^2)$ bins for $\beta$ = 2, inclusive in $p_T$.
Measurements of jet substructure describing the composition of quark- and gluon-initiated jets are presented. Proton-proton (pp) collision data at $\sqrt{s}$ =13 TeV collected with the CMS detector are used, corresponding to an integrated luminosity of 35.9 fb$^{-1}$. Generalized angularities are measured that characterize the jet substructure and distinguish quark- and gluon-initiated jets. These observables are sensitive to the distributions of transverse momenta and angular distances within a jet. The analysis is performed using a data sample of dijet events enriched in gluon-initiated jets, and, for the first time, a Z+jet event sample enriched in quark-initiated jets. The observables are measured in bins of jet transverse momentum, and as a function of the jet radius parameter. Each measurement is repeated applying a "soft drop" grooming procedure that removes soft and large angle radiation from the jet. Using these measurements, the ability of various models to describe jet substructure is assessed, showing a clear need for improvements in Monte Carlo generators.
Particle-level distributions of ungroomed AK4 multiplicity in 120 < PT < 150 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 multiplicity in 120 < PT < 150 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 pTD2 in 120 < PT < 150 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 pTD2 in 120 < PT < 150 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 thrust in 120 < PT < 150 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 thrust in 120 < PT < 150 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 width in 120 < PT < 150 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 width in 120 < PT < 150 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 LHA in 120 < PT < 150 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 LHA in 120 < PT < 150 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 LHA in 408 < PT < 1500 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 LHA in 1000 < PT < 4000 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 LHA in 120 < PT < 150 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 LHA in 120 < PT < 150 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 LHA (charged-only) in 120 < PT < 150 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 LHA (charged-only) in 120 < PT < 150 GeV in the central dijet region.
Particle-level distributions of groomed AK4 LHA in 120 < PT < 150 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 LHA in 120 < PT < 150 GeV in the central dijet region.
Mean of ungroomed LHA for AK4 jets as a function of PT in the Z+jet region.
Mean of ungroomed LHA for AK4 jets as a function of PT in the central dijet region.
Mean of ungroomed LHA for AK4 jets as a function of PT in the forward dijet region.
Mean of ungroomed LHA (charged-only) for AK4 jets as a function of PT in the Z+jet region.
Mean of ungroomed LHA (charged-only) for AK4 jets as a function of PT in the central dijet region.
Mean of ungroomed LHA (charged-only) for AK4 jets as a function of PT in the forward dijet region.
Mean of ungroomed multiplicity (charged-only) for AK4 jets as a function of PT in the Z+jet region.
Mean of ungroomed multiplicity (charged-only) for AK4 jets as a function of PT in the central dijet region.
Mean of ungroomed multiplicity (charged-only) for AK4 jets as a function of PT in the forward dijet region.
Mean of ungroomed pTD2 (charged-only) for AK4 jets as a function of PT in the Z+jet region.
Mean of ungroomed pTD2 (charged-only) for AK4 jets as a function of PT in the central dijet region.
Mean of ungroomed pTD2 (charged-only) for AK4 jets as a function of PT in the forward dijet region.
Mean of ungroomed thrust (charged-only) for AK4 jets as a function of PT in the Z+jet region.
Mean of ungroomed thrust (charged-only) for AK4 jets as a function of PT in the central dijet region.
Mean of ungroomed thrust (charged-only) for AK4 jets as a function of PT in the forward dijet region.
Mean of ungroomed width (charged-only) for AK4 jets as a function of PT in the Z+jet region.
Mean of ungroomed width (charged-only) for AK4 jets as a function of PT in the central dijet region.
Mean of ungroomed width (charged-only) for AK4 jets as a function of PT in the forward dijet region.
Mean of ungroomed multiplicity for AK4 jets as a function of PT in the Z+jet region.
Mean of ungroomed multiplicity for AK4 jets as a function of PT in the central dijet region.
Mean of ungroomed multiplicity for AK4 jets as a function of PT in the forward dijet region.
Mean of ungroomed pTD2 for AK4 jets as a function of PT in the Z+jet region.
Mean of ungroomed pTD2 for AK4 jets as a function of PT in the central dijet region.
Mean of ungroomed pTD2 for AK4 jets as a function of PT in the forward dijet region.
Mean of ungroomed thrust for AK4 jets as a function of PT in the Z+jet region.
Mean of ungroomed thrust for AK4 jets as a function of PT in the central dijet region.
Mean of ungroomed thrust for AK4 jets as a function of PT in the forward dijet region.
Mean of ungroomed width for AK4 jets as a function of PT in the Z+jet region.
Mean of ungroomed width for AK4 jets as a function of PT in the central dijet region.
Mean of ungroomed width for AK4 jets as a function of PT in the forward dijet region.
Mean of groomed LHA for AK4 jets as a function of PT in the Z+jet region.
Mean of groomed LHA for AK4 jets as a function of PT in the central dijet region.
Mean of groomed LHA for AK4 jets as a function of PT in the forward dijet region.
Mean of groomed LHA (charged-only) for AK4 jets as a function of PT in the Z+jet region.
Mean of groomed LHA (charged-only) for AK4 jets as a function of PT in the central dijet region.
Mean of groomed LHA (charged-only) for AK4 jets as a function of PT in the forward dijet region.
Mean of groomed multiplicity (charged-only) for AK4 jets as a function of PT in the Z+jet region.
Mean of groomed multiplicity (charged-only) for AK4 jets as a function of PT in the central dijet region.
Mean of groomed multiplicity (charged-only) for AK4 jets as a function of PT in the forward dijet region.
Mean of groomed pTD2 (charged-only) for AK4 jets as a function of PT in the Z+jet region.
Mean of groomed pTD2 (charged-only) for AK4 jets as a function of PT in the central dijet region.
Mean of groomed pTD2 (charged-only) for AK4 jets as a function of PT in the forward dijet region.
Mean of groomed thrust (charged-only) for AK4 jets as a function of PT in the Z+jet region.
Mean of groomed thrust (charged-only) for AK4 jets as a function of PT in the central dijet region.
Mean of groomed thrust (charged-only) for AK4 jets as a function of PT in the forward dijet region.
Mean of groomed width (charged-only) for AK4 jets as a function of PT in the Z+jet region.
Mean of groomed width (charged-only) for AK4 jets as a function of PT in the central dijet region.
Mean of groomed width (charged-only) for AK4 jets as a function of PT in the forward dijet region.
Mean of groomed multiplicity for AK4 jets as a function of PT in the Z+jet region.
Mean of groomed multiplicity for AK4 jets as a function of PT in the central dijet region.
Mean of groomed multiplicity for AK4 jets as a function of PT in the forward dijet region.
Mean of groomed pTD2 for AK4 jets as a function of PT in the Z+jet region.
Mean of groomed pTD2 for AK4 jets as a function of PT in the central dijet region.
Mean of groomed pTD2 for AK4 jets as a function of PT in the forward dijet region.
Mean of groomed thrust for AK4 jets as a function of PT in the Z+jet region.
Mean of groomed thrust for AK4 jets as a function of PT in the central dijet region.
Mean of groomed thrust for AK4 jets as a function of PT in the forward dijet region.
Mean of groomed width for AK4 jets as a function of PT in the Z+jet region.
Mean of groomed width for AK4 jets as a function of PT in the central dijet region.
Mean of groomed width for AK4 jets as a function of PT in the forward dijet region.
Mean of ungroomed LHA for AK8 jets as a function of PT in the Z+jet region.
Mean of ungroomed LHA for AK8 jets as a function of PT in the central dijet region.
Mean of ungroomed LHA for AK8 jets as a function of PT in the forward dijet region.
Mean of ungroomed LHA (charged-only) for AK8 jets as a function of PT in the Z+jet region.
Mean of ungroomed LHA (charged-only) for AK8 jets as a function of PT in the central dijet region.
Mean of ungroomed LHA (charged-only) for AK8 jets as a function of PT in the forward dijet region.
Mean of ungroomed multiplicity (charged-only) for AK8 jets as a function of PT in the Z+jet region.
Mean of ungroomed multiplicity (charged-only) for AK8 jets as a function of PT in the central dijet region.
Mean of ungroomed multiplicity (charged-only) for AK8 jets as a function of PT in the forward dijet region.
Mean of ungroomed pTD2 (charged-only) for AK8 jets as a function of PT in the Z+jet region.
Mean of ungroomed pTD2 (charged-only) for AK8 jets as a function of PT in the central dijet region.
Mean of ungroomed pTD2 (charged-only) for AK8 jets as a function of PT in the forward dijet region.
Mean of ungroomed thrust (charged-only) for AK8 jets as a function of PT in the Z+jet region.
Mean of ungroomed thrust (charged-only) for AK8 jets as a function of PT in the central dijet region.
Mean of ungroomed thrust (charged-only) for AK8 jets as a function of PT in the forward dijet region.
Mean of ungroomed width (charged-only) for AK8 jets as a function of PT in the Z+jet region.
Mean of ungroomed width (charged-only) for AK8 jets as a function of PT in the central dijet region.
Mean of ungroomed width (charged-only) for AK8 jets as a function of PT in the forward dijet region.
Mean of ungroomed multiplicity for AK8 jets as a function of PT in the Z+jet region.
Mean of ungroomed multiplicity for AK8 jets as a function of PT in the central dijet region.
Mean of ungroomed multiplicity for AK8 jets as a function of PT in the forward dijet region.
Mean of ungroomed pTD2 for AK8 jets as a function of PT in the Z+jet region.
Mean of ungroomed pTD2 for AK8 jets as a function of PT in the central dijet region.
Mean of ungroomed pTD2 for AK8 jets as a function of PT in the forward dijet region.
Mean of ungroomed thrust for AK8 jets as a function of PT in the Z+jet region.
Mean of ungroomed thrust for AK8 jets as a function of PT in the central dijet region.
Mean of ungroomed thrust for AK8 jets as a function of PT in the forward dijet region.
Mean of ungroomed width for AK8 jets as a function of PT in the Z+jet region.
Mean of ungroomed width for AK8 jets as a function of PT in the central dijet region.
Mean of ungroomed width for AK8 jets as a function of PT in the forward dijet region.
Mean of groomed LHA for AK8 jets as a function of PT in the Z+jet region.
Mean of groomed LHA for AK8 jets as a function of PT in the central dijet region.
Mean of groomed LHA for AK8 jets as a function of PT in the forward dijet region.
Mean of groomed LHA (charged-only) for AK8 jets as a function of PT in the Z+jet region.
Mean of groomed LHA (charged-only) for AK8 jets as a function of PT in the central dijet region.
Mean of groomed LHA (charged-only) for AK8 jets as a function of PT in the forward dijet region.
Mean of groomed multiplicity (charged-only) for AK8 jets as a function of PT in the Z+jet region.
Mean of groomed multiplicity (charged-only) for AK8 jets as a function of PT in the central dijet region.
Mean of groomed multiplicity (charged-only) for AK8 jets as a function of PT in the forward dijet region.
Mean of groomed pTD2 (charged-only) for AK8 jets as a function of PT in the Z+jet region.
Mean of groomed pTD2 (charged-only) for AK8 jets as a function of PT in the central dijet region.
Mean of groomed pTD2 (charged-only) for AK8 jets as a function of PT in the forward dijet region.
Mean of groomed thrust (charged-only) for AK8 jets as a function of PT in the Z+jet region.
Mean of groomed thrust (charged-only) for AK8 jets as a function of PT in the central dijet region.
Mean of groomed thrust (charged-only) for AK8 jets as a function of PT in the forward dijet region.
Mean of groomed width (charged-only) for AK8 jets as a function of PT in the Z+jet region.
Mean of groomed width (charged-only) for AK8 jets as a function of PT in the central dijet region.
Mean of groomed width (charged-only) for AK8 jets as a function of PT in the forward dijet region.
Mean of groomed multiplicity for AK8 jets as a function of PT in the Z+jet region.
Mean of groomed multiplicity for AK8 jets as a function of PT in the central dijet region.
Mean of groomed multiplicity for AK8 jets as a function of PT in the forward dijet region.
Mean of groomed pTD2 for AK8 jets as a function of PT in the Z+jet region.
Mean of groomed pTD2 for AK8 jets as a function of PT in the central dijet region.
Mean of groomed pTD2 for AK8 jets as a function of PT in the forward dijet region.
Mean of groomed thrust for AK8 jets as a function of PT in the Z+jet region.
Mean of groomed thrust for AK8 jets as a function of PT in the central dijet region.
Mean of groomed thrust for AK8 jets as a function of PT in the forward dijet region.
Mean of groomed width for AK8 jets as a function of PT in the Z+jet region.
Mean of groomed width for AK8 jets as a function of PT in the central dijet region.
Mean of groomed width for AK8 jets as a function of PT in the forward dijet region.
Particle-level distributions of ungroomed AK4 LHA in 50 < PT < 65 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 LHA in 65 < PT < 88 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 LHA in 88 < PT < 120 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 LHA in 150 < PT < 186 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 LHA in 186 < PT < 254 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 LHA in 254 < PT < 326 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 LHA in 326 < PT < 408 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 LHA in 50 < PT < 65 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 LHA in 65 < PT < 88 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 LHA in 88 < PT < 120 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 LHA in 120 < PT < 150 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 LHA in 150 < PT < 186 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 LHA in 186 < PT < 254 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 LHA in 254 < PT < 326 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 LHA in 326 < PT < 408 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 LHA in 408 < PT < 1500 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 LHA in 50 < PT < 65 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 LHA in 65 < PT < 88 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 LHA in 88 < PT < 120 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 LHA in 150 < PT < 186 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 LHA in 186 < PT < 254 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 LHA in 254 < PT < 326 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 LHA in 326 < PT < 408 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 LHA in 408 < PT < 481 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 LHA in 481 < PT < 614 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 LHA in 614 < PT < 800 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 LHA in 800 < PT < 1000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 LHA in 50 < PT < 65 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 LHA in 65 < PT < 88 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 LHA in 88 < PT < 120 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 LHA in 120 < PT < 150 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 LHA in 150 < PT < 186 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 LHA in 186 < PT < 254 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 LHA in 254 < PT < 326 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 LHA in 326 < PT < 408 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 LHA in 408 < PT < 481 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 LHA in 481 < PT < 614 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 LHA in 614 < PT < 800 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 LHA in 800 < PT < 1000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 LHA in 1000 < PT < 4000 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 LHA in 50 < PT < 65 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 LHA in 65 < PT < 88 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 LHA in 88 < PT < 120 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 LHA in 120 < PT < 150 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 LHA in 150 < PT < 186 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 LHA in 186 < PT < 254 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 LHA in 254 < PT < 326 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 LHA in 326 < PT < 408 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 LHA in 408 < PT < 481 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 LHA in 481 < PT < 614 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 LHA in 614 < PT < 800 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 LHA in 800 < PT < 1000 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 LHA in 1000 < PT < 4000 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 LHA (charged-only) in 50 < PT < 65 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 LHA (charged-only) in 65 < PT < 88 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 LHA (charged-only) in 88 < PT < 120 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 LHA (charged-only) in 150 < PT < 186 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 LHA (charged-only) in 186 < PT < 254 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 LHA (charged-only) in 254 < PT < 326 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 LHA (charged-only) in 326 < PT < 408 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 LHA (charged-only) in 408 < PT < 1500 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 LHA (charged-only) in 50 < PT < 65 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 LHA (charged-only) in 65 < PT < 88 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 LHA (charged-only) in 88 < PT < 120 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 LHA (charged-only) in 120 < PT < 150 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 LHA (charged-only) in 150 < PT < 186 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 LHA (charged-only) in 186 < PT < 254 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 LHA (charged-only) in 254 < PT < 326 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 LHA (charged-only) in 326 < PT < 408 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 LHA (charged-only) in 408 < PT < 1500 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 LHA (charged-only) in 50 < PT < 65 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 LHA (charged-only) in 65 < PT < 88 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 LHA (charged-only) in 88 < PT < 120 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 LHA (charged-only) in 150 < PT < 186 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 LHA (charged-only) in 186 < PT < 254 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 LHA (charged-only) in 254 < PT < 326 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 LHA (charged-only) in 326 < PT < 408 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 LHA (charged-only) in 408 < PT < 481 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 LHA (charged-only) in 481 < PT < 614 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 LHA (charged-only) in 614 < PT < 800 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 LHA (charged-only) in 800 < PT < 1000 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 LHA (charged-only) in 1000 < PT < 4000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 LHA (charged-only) in 50 < PT < 65 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 LHA (charged-only) in 65 < PT < 88 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 LHA (charged-only) in 88 < PT < 120 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 LHA (charged-only) in 120 < PT < 150 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 LHA (charged-only) in 150 < PT < 186 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 LHA (charged-only) in 186 < PT < 254 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 LHA (charged-only) in 254 < PT < 326 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 LHA (charged-only) in 326 < PT < 408 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 LHA (charged-only) in 408 < PT < 481 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 LHA (charged-only) in 481 < PT < 614 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 LHA (charged-only) in 614 < PT < 800 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 LHA (charged-only) in 800 < PT < 1000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 LHA (charged-only) in 1000 < PT < 4000 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 LHA (charged-only) in 50 < PT < 65 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 LHA (charged-only) in 65 < PT < 88 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 LHA (charged-only) in 88 < PT < 120 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 LHA (charged-only) in 120 < PT < 150 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 LHA (charged-only) in 150 < PT < 186 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 LHA (charged-only) in 186 < PT < 254 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 LHA (charged-only) in 254 < PT < 326 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 LHA (charged-only) in 326 < PT < 408 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 LHA (charged-only) in 408 < PT < 481 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 LHA (charged-only) in 481 < PT < 614 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 LHA (charged-only) in 614 < PT < 800 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 LHA (charged-only) in 800 < PT < 1000 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 LHA (charged-only) in 1000 < PT < 4000 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 50 < PT < 65 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 65 < PT < 88 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 88 < PT < 120 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 120 < PT < 150 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 150 < PT < 186 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 186 < PT < 254 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 254 < PT < 326 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 326 < PT < 408 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 408 < PT < 1500 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 50 < PT < 65 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 65 < PT < 88 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 88 < PT < 120 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 120 < PT < 150 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 150 < PT < 186 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 186 < PT < 254 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 254 < PT < 326 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 326 < PT < 408 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 408 < PT < 1500 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 50 < PT < 65 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 65 < PT < 88 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 88 < PT < 120 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 120 < PT < 150 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 150 < PT < 186 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 186 < PT < 254 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 254 < PT < 326 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 326 < PT < 408 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 408 < PT < 481 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 481 < PT < 614 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 614 < PT < 800 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 800 < PT < 1000 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 1000 < PT < 4000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 50 < PT < 65 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 65 < PT < 88 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 88 < PT < 120 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 120 < PT < 150 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 150 < PT < 186 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 186 < PT < 254 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 254 < PT < 326 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 326 < PT < 408 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 408 < PT < 481 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 481 < PT < 614 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 614 < PT < 800 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 800 < PT < 1000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 1000 < PT < 4000 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 50 < PT < 65 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 65 < PT < 88 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 88 < PT < 120 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 120 < PT < 150 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 150 < PT < 186 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 186 < PT < 254 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 254 < PT < 326 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 326 < PT < 408 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 408 < PT < 481 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 481 < PT < 614 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 614 < PT < 800 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 800 < PT < 1000 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 1000 < PT < 4000 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 50 < PT < 65 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 65 < PT < 88 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 88 < PT < 120 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 120 < PT < 150 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 150 < PT < 186 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 186 < PT < 254 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 254 < PT < 326 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 326 < PT < 408 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 408 < PT < 1500 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 50 < PT < 65 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 65 < PT < 88 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 88 < PT < 120 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 120 < PT < 150 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 150 < PT < 186 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 186 < PT < 254 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 254 < PT < 326 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 326 < PT < 408 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 408 < PT < 1500 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 50 < PT < 65 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 65 < PT < 88 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 88 < PT < 120 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 120 < PT < 150 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 150 < PT < 186 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 186 < PT < 254 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 254 < PT < 326 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 326 < PT < 408 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 408 < PT < 481 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 481 < PT < 614 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 614 < PT < 800 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 800 < PT < 1000 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 1000 < PT < 4000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 50 < PT < 65 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 65 < PT < 88 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 88 < PT < 120 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 120 < PT < 150 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 150 < PT < 186 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 186 < PT < 254 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 254 < PT < 326 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 326 < PT < 408 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 408 < PT < 481 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 481 < PT < 614 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 614 < PT < 800 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 800 < PT < 1000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 1000 < PT < 4000 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 50 < PT < 65 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 65 < PT < 88 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 88 < PT < 120 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 120 < PT < 150 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 150 < PT < 186 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 186 < PT < 254 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 254 < PT < 326 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 326 < PT < 408 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 408 < PT < 481 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 481 < PT < 614 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 614 < PT < 800 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 800 < PT < 1000 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 1000 < PT < 4000 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 50 < PT < 65 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 65 < PT < 88 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 88 < PT < 120 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 120 < PT < 150 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 150 < PT < 186 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 186 < PT < 254 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 254 < PT < 326 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 326 < PT < 408 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 408 < PT < 1500 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust (charged-only) in 50 < PT < 65 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust (charged-only) in 65 < PT < 88 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust (charged-only) in 88 < PT < 120 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust (charged-only) in 120 < PT < 150 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust (charged-only) in 150 < PT < 186 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust (charged-only) in 186 < PT < 254 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust (charged-only) in 254 < PT < 326 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust (charged-only) in 326 < PT < 408 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust (charged-only) in 408 < PT < 1500 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 50 < PT < 65 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 65 < PT < 88 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 88 < PT < 120 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 120 < PT < 150 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 150 < PT < 186 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 186 < PT < 254 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 254 < PT < 326 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 326 < PT < 408 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 408 < PT < 481 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 481 < PT < 614 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 614 < PT < 800 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 800 < PT < 1000 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 1000 < PT < 4000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust (charged-only) in 50 < PT < 65 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust (charged-only) in 65 < PT < 88 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust (charged-only) in 88 < PT < 120 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust (charged-only) in 120 < PT < 150 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust (charged-only) in 150 < PT < 186 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust (charged-only) in 186 < PT < 254 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust (charged-only) in 254 < PT < 326 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust (charged-only) in 326 < PT < 408 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust (charged-only) in 408 < PT < 481 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust (charged-only) in 481 < PT < 614 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust (charged-only) in 614 < PT < 800 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust (charged-only) in 800 < PT < 1000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust (charged-only) in 1000 < PT < 4000 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 50 < PT < 65 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 65 < PT < 88 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 88 < PT < 120 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 120 < PT < 150 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 150 < PT < 186 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 186 < PT < 254 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 254 < PT < 326 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 326 < PT < 408 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 408 < PT < 481 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 481 < PT < 614 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 614 < PT < 800 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 800 < PT < 1000 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 1000 < PT < 4000 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 50 < PT < 65 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 65 < PT < 88 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 88 < PT < 120 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 120 < PT < 150 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 150 < PT < 186 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 186 < PT < 254 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 254 < PT < 326 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 326 < PT < 408 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 408 < PT < 1500 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width (charged-only) in 50 < PT < 65 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width (charged-only) in 65 < PT < 88 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width (charged-only) in 88 < PT < 120 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width (charged-only) in 120 < PT < 150 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width (charged-only) in 150 < PT < 186 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width (charged-only) in 186 < PT < 254 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width (charged-only) in 254 < PT < 326 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width (charged-only) in 326 < PT < 408 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width (charged-only) in 408 < PT < 1500 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 50 < PT < 65 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 65 < PT < 88 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 88 < PT < 120 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 120 < PT < 150 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 150 < PT < 186 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 186 < PT < 254 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 254 < PT < 326 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 326 < PT < 408 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 408 < PT < 481 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 481 < PT < 614 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 614 < PT < 800 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 800 < PT < 1000 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 1000 < PT < 4000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width (charged-only) in 50 < PT < 65 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width (charged-only) in 65 < PT < 88 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width (charged-only) in 88 < PT < 120 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width (charged-only) in 120 < PT < 150 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width (charged-only) in 150 < PT < 186 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width (charged-only) in 186 < PT < 254 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width (charged-only) in 254 < PT < 326 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width (charged-only) in 326 < PT < 408 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width (charged-only) in 408 < PT < 481 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width (charged-only) in 481 < PT < 614 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width (charged-only) in 614 < PT < 800 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width (charged-only) in 800 < PT < 1000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width (charged-only) in 1000 < PT < 4000 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 50 < PT < 65 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 65 < PT < 88 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 88 < PT < 120 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 120 < PT < 150 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 150 < PT < 186 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 186 < PT < 254 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 254 < PT < 326 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 326 < PT < 408 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 408 < PT < 481 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 481 < PT < 614 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 614 < PT < 800 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 800 < PT < 1000 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 1000 < PT < 4000 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 multiplicity in 50 < PT < 65 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 multiplicity in 65 < PT < 88 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 multiplicity in 88 < PT < 120 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 multiplicity in 150 < PT < 186 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 multiplicity in 186 < PT < 254 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 multiplicity in 254 < PT < 326 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 multiplicity in 326 < PT < 408 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 multiplicity in 408 < PT < 1500 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity in 50 < PT < 65 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity in 65 < PT < 88 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity in 88 < PT < 120 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity in 120 < PT < 150 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity in 150 < PT < 186 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity in 186 < PT < 254 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity in 254 < PT < 326 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity in 326 < PT < 408 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity in 408 < PT < 1500 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 multiplicity in 50 < PT < 65 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 multiplicity in 65 < PT < 88 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 multiplicity in 88 < PT < 120 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 multiplicity in 150 < PT < 186 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 multiplicity in 186 < PT < 254 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 multiplicity in 254 < PT < 326 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 multiplicity in 326 < PT < 408 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 multiplicity in 408 < PT < 481 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 multiplicity in 481 < PT < 614 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 multiplicity in 614 < PT < 800 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 multiplicity in 800 < PT < 1000 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 multiplicity in 1000 < PT < 4000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity in 50 < PT < 65 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity in 65 < PT < 88 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity in 88 < PT < 120 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity in 120 < PT < 150 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity in 150 < PT < 186 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity in 186 < PT < 254 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity in 254 < PT < 326 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity in 326 < PT < 408 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity in 408 < PT < 481 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity in 481 < PT < 614 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity in 614 < PT < 800 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity in 800 < PT < 1000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity in 1000 < PT < 4000 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 multiplicity in 50 < PT < 65 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 multiplicity in 65 < PT < 88 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 multiplicity in 88 < PT < 120 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 multiplicity in 120 < PT < 150 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 multiplicity in 150 < PT < 186 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 multiplicity in 186 < PT < 254 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 multiplicity in 254 < PT < 326 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 multiplicity in 326 < PT < 408 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 multiplicity in 408 < PT < 481 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 multiplicity in 481 < PT < 614 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 multiplicity in 614 < PT < 800 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 multiplicity in 800 < PT < 1000 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 multiplicity in 1000 < PT < 4000 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 pTD2 in 50 < PT < 65 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 pTD2 in 65 < PT < 88 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 pTD2 in 88 < PT < 120 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 pTD2 in 150 < PT < 186 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 pTD2 in 186 < PT < 254 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 pTD2 in 254 < PT < 326 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 pTD2 in 326 < PT < 408 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 pTD2 in 408 < PT < 1500 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 in 50 < PT < 65 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 in 65 < PT < 88 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 in 88 < PT < 120 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 in 120 < PT < 150 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 in 150 < PT < 186 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 in 186 < PT < 254 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 in 254 < PT < 326 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 in 326 < PT < 408 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 in 408 < PT < 1500 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 pTD2 in 50 < PT < 65 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 pTD2 in 65 < PT < 88 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 pTD2 in 88 < PT < 120 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 pTD2 in 150 < PT < 186 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 pTD2 in 186 < PT < 254 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 pTD2 in 254 < PT < 326 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 pTD2 in 326 < PT < 408 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 pTD2 in 408 < PT < 481 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 pTD2 in 481 < PT < 614 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 pTD2 in 614 < PT < 800 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 pTD2 in 800 < PT < 1000 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 pTD2 in 1000 < PT < 4000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 in 50 < PT < 65 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 in 65 < PT < 88 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 in 88 < PT < 120 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 in 120 < PT < 150 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 in 150 < PT < 186 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 in 186 < PT < 254 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 in 254 < PT < 326 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 in 326 < PT < 408 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 in 408 < PT < 481 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 in 481 < PT < 614 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 in 614 < PT < 800 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 in 800 < PT < 1000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 in 1000 < PT < 4000 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 pTD2 in 50 < PT < 65 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 pTD2 in 65 < PT < 88 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 pTD2 in 88 < PT < 120 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 pTD2 in 120 < PT < 150 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 pTD2 in 150 < PT < 186 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 pTD2 in 186 < PT < 254 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 pTD2 in 254 < PT < 326 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 pTD2 in 326 < PT < 408 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 pTD2 in 408 < PT < 481 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 pTD2 in 481 < PT < 614 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 pTD2 in 614 < PT < 800 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 pTD2 in 800 < PT < 1000 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 pTD2 in 1000 < PT < 4000 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 thrust in 50 < PT < 65 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 thrust in 65 < PT < 88 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 thrust in 88 < PT < 120 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 thrust in 150 < PT < 186 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 thrust in 186 < PT < 254 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 thrust in 254 < PT < 326 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 thrust in 326 < PT < 408 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 thrust in 408 < PT < 1500 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust in 50 < PT < 65 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust in 65 < PT < 88 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust in 88 < PT < 120 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust in 120 < PT < 150 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust in 150 < PT < 186 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust in 186 < PT < 254 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust in 254 < PT < 326 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust in 326 < PT < 408 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust in 408 < PT < 1500 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 thrust in 50 < PT < 65 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 thrust in 65 < PT < 88 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 thrust in 88 < PT < 120 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 thrust in 150 < PT < 186 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 thrust in 186 < PT < 254 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 thrust in 254 < PT < 326 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 thrust in 326 < PT < 408 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 thrust in 408 < PT < 481 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 thrust in 481 < PT < 614 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 thrust in 614 < PT < 800 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 thrust in 800 < PT < 1000 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 thrust in 1000 < PT < 4000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust in 50 < PT < 65 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust in 65 < PT < 88 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust in 88 < PT < 120 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust in 120 < PT < 150 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust in 150 < PT < 186 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust in 186 < PT < 254 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust in 254 < PT < 326 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust in 326 < PT < 408 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust in 408 < PT < 481 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust in 481 < PT < 614 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust in 614 < PT < 800 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust in 800 < PT < 1000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust in 1000 < PT < 4000 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 thrust in 50 < PT < 65 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 thrust in 65 < PT < 88 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 thrust in 88 < PT < 120 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 thrust in 120 < PT < 150 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 thrust in 150 < PT < 186 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 thrust in 186 < PT < 254 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 thrust in 254 < PT < 326 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 thrust in 326 < PT < 408 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 thrust in 408 < PT < 481 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 thrust in 481 < PT < 614 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 thrust in 614 < PT < 800 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 thrust in 800 < PT < 1000 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 thrust in 1000 < PT < 4000 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 width in 50 < PT < 65 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 width in 65 < PT < 88 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 width in 88 < PT < 120 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 width in 150 < PT < 186 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 width in 186 < PT < 254 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 width in 254 < PT < 326 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 width in 326 < PT < 408 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 width in 408 < PT < 1500 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width in 50 < PT < 65 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width in 65 < PT < 88 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width in 88 < PT < 120 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width in 120 < PT < 150 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width in 150 < PT < 186 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width in 186 < PT < 254 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width in 254 < PT < 326 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width in 326 < PT < 408 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width in 408 < PT < 1500 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 width in 50 < PT < 65 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 width in 65 < PT < 88 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 width in 88 < PT < 120 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 width in 150 < PT < 186 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 width in 186 < PT < 254 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 width in 254 < PT < 326 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 width in 326 < PT < 408 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 width in 408 < PT < 481 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 width in 481 < PT < 614 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 width in 614 < PT < 800 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 width in 800 < PT < 1000 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 width in 1000 < PT < 4000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width in 50 < PT < 65 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width in 65 < PT < 88 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width in 88 < PT < 120 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width in 120 < PT < 150 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width in 150 < PT < 186 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width in 186 < PT < 254 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width in 254 < PT < 326 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width in 326 < PT < 408 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width in 408 < PT < 481 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width in 481 < PT < 614 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width in 614 < PT < 800 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width in 800 < PT < 1000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width in 1000 < PT < 4000 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 width in 50 < PT < 65 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 width in 65 < PT < 88 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 width in 88 < PT < 120 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 width in 120 < PT < 150 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 width in 150 < PT < 186 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 width in 186 < PT < 254 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 width in 254 < PT < 326 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 width in 326 < PT < 408 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 width in 408 < PT < 481 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 width in 481 < PT < 614 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 width in 614 < PT < 800 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 width in 800 < PT < 1000 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 width in 1000 < PT < 4000 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 LHA in 50 < PT < 65 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 LHA in 65 < PT < 88 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 LHA in 88 < PT < 120 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 LHA in 150 < PT < 186 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 LHA in 186 < PT < 254 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 LHA in 254 < PT < 326 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 LHA in 326 < PT < 408 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 LHA in 408 < PT < 1500 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA in 50 < PT < 65 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA in 65 < PT < 88 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA in 88 < PT < 120 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA in 120 < PT < 150 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA in 150 < PT < 186 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA in 186 < PT < 254 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA in 254 < PT < 326 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA in 326 < PT < 408 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA in 408 < PT < 1500 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 LHA in 50 < PT < 65 GeV in the central dijet region.
Particle-level distributions of groomed AK4 LHA in 65 < PT < 88 GeV in the central dijet region.
Particle-level distributions of groomed AK4 LHA in 88 < PT < 120 GeV in the central dijet region.
Particle-level distributions of groomed AK4 LHA in 150 < PT < 186 GeV in the central dijet region.
Particle-level distributions of groomed AK4 LHA in 186 < PT < 254 GeV in the central dijet region.
Particle-level distributions of groomed AK4 LHA in 254 < PT < 326 GeV in the central dijet region.
Particle-level distributions of groomed AK4 LHA in 326 < PT < 408 GeV in the central dijet region.
Particle-level distributions of groomed AK4 LHA in 408 < PT < 481 GeV in the central dijet region.
Particle-level distributions of groomed AK4 LHA in 481 < PT < 614 GeV in the central dijet region.
Particle-level distributions of groomed AK4 LHA in 614 < PT < 800 GeV in the central dijet region.
Particle-level distributions of groomed AK4 LHA in 800 < PT < 1000 GeV in the central dijet region.
Particle-level distributions of groomed AK4 LHA in 1000 < PT < 4000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA in 50 < PT < 65 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA in 65 < PT < 88 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA in 88 < PT < 120 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA in 120 < PT < 150 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA in 150 < PT < 186 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA in 186 < PT < 254 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA in 254 < PT < 326 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA in 326 < PT < 408 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA in 408 < PT < 481 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA in 481 < PT < 614 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA in 614 < PT < 800 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA in 800 < PT < 1000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA in 1000 < PT < 4000 GeV in the central dijet region.
Particle-level distributions of groomed AK4 LHA in 50 < PT < 65 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 LHA in 65 < PT < 88 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 LHA in 88 < PT < 120 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 LHA in 120 < PT < 150 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 LHA in 150 < PT < 186 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 LHA in 186 < PT < 254 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 LHA in 254 < PT < 326 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 LHA in 326 < PT < 408 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 LHA in 408 < PT < 481 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 LHA in 481 < PT < 614 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 LHA in 614 < PT < 800 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 LHA in 800 < PT < 1000 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 LHA in 1000 < PT < 4000 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 50 < PT < 65 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 65 < PT < 88 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 88 < PT < 120 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 120 < PT < 150 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 150 < PT < 186 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 186 < PT < 254 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 254 < PT < 326 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 326 < PT < 408 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 408 < PT < 1500 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA (charged-only) in 50 < PT < 65 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA (charged-only) in 65 < PT < 88 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA (charged-only) in 88 < PT < 120 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA (charged-only) in 120 < PT < 150 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA (charged-only) in 150 < PT < 186 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA (charged-only) in 186 < PT < 254 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA (charged-only) in 254 < PT < 326 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA (charged-only) in 326 < PT < 408 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA (charged-only) in 408 < PT < 1500 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 50 < PT < 65 GeV in the central dijet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 65 < PT < 88 GeV in the central dijet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 88 < PT < 120 GeV in the central dijet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 120 < PT < 150 GeV in the central dijet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 150 < PT < 186 GeV in the central dijet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 186 < PT < 254 GeV in the central dijet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 254 < PT < 326 GeV in the central dijet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 326 < PT < 408 GeV in the central dijet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 408 < PT < 481 GeV in the central dijet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 481 < PT < 614 GeV in the central dijet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 614 < PT < 800 GeV in the central dijet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 800 < PT < 1000 GeV in the central dijet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 1000 < PT < 4000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA (charged-only) in 50 < PT < 65 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA (charged-only) in 65 < PT < 88 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA (charged-only) in 88 < PT < 120 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA (charged-only) in 120 < PT < 150 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA (charged-only) in 150 < PT < 186 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA (charged-only) in 186 < PT < 254 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA (charged-only) in 254 < PT < 326 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA (charged-only) in 326 < PT < 408 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA (charged-only) in 408 < PT < 481 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA (charged-only) in 481 < PT < 614 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA (charged-only) in 614 < PT < 800 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA (charged-only) in 800 < PT < 1000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA (charged-only) in 1000 < PT < 4000 GeV in the central dijet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 50 < PT < 65 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 65 < PT < 88 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 88 < PT < 120 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 120 < PT < 150 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 150 < PT < 186 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 186 < PT < 254 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 254 < PT < 326 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 326 < PT < 408 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 408 < PT < 481 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 481 < PT < 614 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 614 < PT < 800 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 800 < PT < 1000 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 1000 < PT < 4000 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 50 < PT < 65 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 65 < PT < 88 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 88 < PT < 120 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 120 < PT < 150 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 150 < PT < 186 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 186 < PT < 254 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 254 < PT < 326 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 326 < PT < 408 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 408 < PT < 1500 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity (charged-only) in 50 < PT < 65 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity (charged-only) in 65 < PT < 88 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity (charged-only) in 88 < PT < 120 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity (charged-only) in 120 < PT < 150 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity (charged-only) in 150 < PT < 186 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity (charged-only) in 186 < PT < 254 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity (charged-only) in 254 < PT < 326 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity (charged-only) in 326 < PT < 408 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity (charged-only) in 408 < PT < 1500 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 50 < PT < 65 GeV in the central dijet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 65 < PT < 88 GeV in the central dijet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 88 < PT < 120 GeV in the central dijet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 120 < PT < 150 GeV in the central dijet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 150 < PT < 186 GeV in the central dijet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 186 < PT < 254 GeV in the central dijet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 254 < PT < 326 GeV in the central dijet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 326 < PT < 408 GeV in the central dijet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 408 < PT < 481 GeV in the central dijet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 481 < PT < 614 GeV in the central dijet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 614 < PT < 800 GeV in the central dijet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 800 < PT < 1000 GeV in the central dijet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 1000 < PT < 4000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity (charged-only) in 50 < PT < 65 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity (charged-only) in 65 < PT < 88 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity (charged-only) in 88 < PT < 120 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity (charged-only) in 120 < PT < 150 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity (charged-only) in 150 < PT < 186 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity (charged-only) in 186 < PT < 254 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity (charged-only) in 254 < PT < 326 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity (charged-only) in 326 < PT < 408 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity (charged-only) in 408 < PT < 481 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity (charged-only) in 481 < PT < 614 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity (charged-only) in 614 < PT < 800 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity (charged-only) in 800 < PT < 1000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity (charged-only) in 1000 < PT < 4000 GeV in the central dijet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 50 < PT < 65 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 65 < PT < 88 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 88 < PT < 120 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 120 < PT < 150 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 150 < PT < 186 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 186 < PT < 254 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 254 < PT < 326 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 326 < PT < 408 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 408 < PT < 481 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 481 < PT < 614 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 614 < PT < 800 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 800 < PT < 1000 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 1000 < PT < 4000 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 pTD2 (charged-only) in 50 < PT < 65 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 pTD2 (charged-only) in 65 < PT < 88 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 pTD2 (charged-only) in 88 < PT < 120 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 pTD2 (charged-only) in 120 < PT < 150 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 pTD2 (charged-only) in 150 < PT < 186 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 pTD2 (charged-only) in 186 < PT < 254 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 pTD2 (charged-only) in 254 < PT < 326 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 pTD2 (charged-only) in 326 < PT < 408 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 pTD2 (charged-only) in 408 < PT < 1500 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 (charged-only) in 50 < PT < 65 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 (charged-only) in 65 < PT < 88 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 (charged-only) in 88 < PT < 120 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 (charged-only) in 120 < PT < 150 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 (charged-only) in 150 < PT < 186 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 (charged-only) in 186 < PT < 254 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 (charged-only) in 254 < PT < 326 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 (charged-only) in 326 < PT < 408 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 (charged-only) in 408 < PT < 1500 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 pTD2 (charged-only) in 50 < PT < 65 GeV in the central dijet region.
Particle-level distributions of groomed AK4 pTD2 (charged-only) in 65 < PT < 88 GeV in the central dijet region.
Particle-level distributions of groomed AK4 pTD2 (charged-only) in 88 < PT < 120 GeV in the central dijet region.
Particle-level distributions of groomed AK4 pTD2 (charged-only) in 120 < PT < 150 GeV in the central dijet region.
Particle-level distributions of groomed AK4 pTD2 (charged-only) in 150 < PT < 186 GeV in the central dijet region.
Particle-level distributions of groomed AK4 pTD2 (charged-only) in 186 < PT < 254 GeV in the central dijet region.
Particle-level distributions of groomed AK4 pTD2 (charged-only) in 254 < PT < 326 GeV in the central dijet region.
Particle-level distributions of groomed AK4 pTD2 (charged-only) in 326 < PT < 408 GeV in the central dijet region.
Particle-level distributions of groomed AK4 pTD2 (charged-only) in 408 < PT < 481 GeV in the central dijet region.
Particle-level distributions of groomed AK4 pTD2 (charged-only) in 481 < PT < 614 GeV in the central dijet region.
Particle-level distributions of groomed AK4 pTD2 (charged-only) in 614 < PT < 800 GeV in the central dijet region.
Particle-level distributions of groomed AK4 pTD2 (charged-only) in 800 < PT < 1000 GeV in the central dijet region.
Particle-level distributions of groomed AK4 pTD2 (charged-only) in 1000 < PT < 4000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 (charged-only) in 50 < PT < 65 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 (charged-only) in 65 < PT < 88 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 (charged-only) in 88 < PT < 120 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 (charged-only) in 120 < PT < 150 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 (charged-only) in 150 < PT < 186 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 (charged-only) in 186 < PT < 254 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 (charged-only) in 254 < PT < 326 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 (charged-only) in 326 < PT < 408 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 (charged-only) in 408 < PT < 481 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 (charged-only) in 481 < PT < 614 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 (charged-only) in 614 < PT < 800 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 (charged-only) in 800 < PT < 1000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 (charged-only) in 1000 < PT < 4000 GeV in the central dijet region.
Particle-level distributions of groomed AK4 pTD2 (charged-only) in 50 < PT < 65 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 pTD2 (charged-only) in 65 < PT < 88 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 pTD2 (charged-only) in 88 < PT < 120 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 pTD2 (charged-only) in 120 < PT < 150 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 pTD2 (charged-only) in 150 < PT < 186 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 pTD2 (charged-only) in 186 < PT < 254 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 pTD2 (charged-only) in 254 < PT < 326 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 pTD2 (charged-only) in 326 < PT < 408 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 pTD2 (charged-only) in 408 < PT < 481 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 pTD2 (charged-only) in 481 < PT < 614 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 pTD2 (charged-only) in 614 < PT < 800 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 pTD2 (charged-only) in 800 < PT < 1000 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 pTD2 (charged-only) in 1000 < PT < 4000 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 thrust (charged-only) in 50 < PT < 65 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 thrust (charged-only) in 65 < PT < 88 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 thrust (charged-only) in 88 < PT < 120 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 thrust (charged-only) in 120 < PT < 150 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 thrust (charged-only) in 150 < PT < 186 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 thrust (charged-only) in 186 < PT < 254 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 thrust (charged-only) in 254 < PT < 326 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 thrust (charged-only) in 326 < PT < 408 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 thrust (charged-only) in 408 < PT < 1500 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 thrust (charged-only) in 50 < PT < 65 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 thrust (charged-only) in 65 < PT < 88 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 thrust (charged-only) in 88 < PT < 120 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 thrust (charged-only) in 120 < PT < 150 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 thrust (charged-only) in 150 < PT < 186 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 thrust (charged-only) in 186 < PT < 254 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 thrust (charged-only) in 254 < PT < 326 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 thrust (charged-only) in 326 < PT < 408 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 thrust (charged-only) in 408 < PT < 1500 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 thrust (charged-only) in 50 < PT < 65 GeV in the central dijet region.
Particle-level distributions of groomed AK4 thrust (charged-only) in 65 < PT < 88 GeV in the central dijet region.
Particle-level distributions of groomed AK4 thrust (charged-only) in 88 < PT < 120 GeV in the central dijet region.
Particle-level distributions of groomed AK4 thrust (charged-only) in 120 < PT < 150 GeV in the central dijet region.
Particle-level distributions of groomed AK4 thrust (charged-only) in 150 < PT < 186 GeV in the central dijet region.
Particle-level distributions of groomed AK4 thrust (charged-only) in 186 < PT < 254 GeV in the central dijet region.
Particle-level distributions of groomed AK4 thrust (charged-only) in 254 < PT < 326 GeV in the central dijet region.
Particle-level distributions of groomed AK4 thrust (charged-only) in 326 < PT < 408 GeV in the central dijet region.
Particle-level distributions of groomed AK4 thrust (charged-only) in 408 < PT < 481 GeV in the central dijet region.
Particle-level distributions of groomed AK4 thrust (charged-only) in 481 < PT < 614 GeV in the central dijet region.
Particle-level distributions of groomed AK4 thrust (charged-only) in 614 < PT < 800 GeV in the central dijet region.
Particle-level distributions of groomed AK4 thrust (charged-only) in 800 < PT < 1000 GeV in the central dijet region.
Particle-level distributions of groomed AK4 thrust (charged-only) in 1000 < PT < 4000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 thrust (charged-only) in 50 < PT < 65 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 thrust (charged-only) in 65 < PT < 88 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 thrust (charged-only) in 88 < PT < 120 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 thrust (charged-only) in 120 < PT < 150 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 thrust (charged-only) in 150 < PT < 186 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 thrust (charged-only) in 186 < PT < 254 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 thrust (charged-only) in 254 < PT < 326 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 thrust (charged-only) in 326 < PT < 408 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 thrust (charged-only) in 408 < PT < 481 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 thrust (charged-only) in 481 < PT < 614 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 thrust (charged-only) in 614 < PT < 800 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 thrust (charged-only) in 800 < PT < 1000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 thrust (charged-only) in 1000 < PT < 4000 GeV in the central dijet region.
Particle-level distributions of groomed AK4 thrust (charged-only) in 50 < PT < 65 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 thrust (charged-only) in 65 < PT < 88 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 thrust (charged-only) in 88 < PT < 120 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 thrust (charged-only) in 120 < PT < 150 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 thrust (charged-only) in 150 < PT < 186 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 thrust (charged-only) in 186 < PT < 254 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 thrust (charged-only) in 254 < PT < 326 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 thrust (charged-only) in 326 < PT < 408 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 thrust (charged-only) in 408 < PT < 481 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 thrust (charged-only) in 481 < PT < 614 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 thrust (charged-only) in 614 < PT < 800 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 thrust (charged-only) in 800 < PT < 1000 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 thrust (charged-only) in 1000 < PT < 4000 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 width (charged-only) in 50 < PT < 65 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 width (charged-only) in 65 < PT < 88 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 width (charged-only) in 88 < PT < 120 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 width (charged-only) in 120 < PT < 150 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 width (charged-only) in 150 < PT < 186 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 width (charged-only) in 186 < PT < 254 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 width (charged-only) in 254 < PT < 326 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 width (charged-only) in 326 < PT < 408 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 width (charged-only) in 408 < PT < 1500 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 width (charged-only) in 50 < PT < 65 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 width (charged-only) in 65 < PT < 88 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 width (charged-only) in 88 < PT < 120 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 width (charged-only) in 120 < PT < 150 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 width (charged-only) in 150 < PT < 186 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 width (charged-only) in 186 < PT < 254 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 width (charged-only) in 254 < PT < 326 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 width (charged-only) in 326 < PT < 408 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 width (charged-only) in 408 < PT < 1500 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 width (charged-only) in 50 < PT < 65 GeV in the central dijet region.
Particle-level distributions of groomed AK4 width (charged-only) in 65 < PT < 88 GeV in the central dijet region.
Particle-level distributions of groomed AK4 width (charged-only) in 88 < PT < 120 GeV in the central dijet region.
Particle-level distributions of groomed AK4 width (charged-only) in 120 < PT < 150 GeV in the central dijet region.
Particle-level distributions of groomed AK4 width (charged-only) in 150 < PT < 186 GeV in the central dijet region.
Particle-level distributions of groomed AK4 width (charged-only) in 186 < PT < 254 GeV in the central dijet region.
Particle-level distributions of groomed AK4 width (charged-only) in 254 < PT < 326 GeV in the central dijet region.
Particle-level distributions of groomed AK4 width (charged-only) in 326 < PT < 408 GeV in the central dijet region.
Particle-level distributions of groomed AK4 width (charged-only) in 408 < PT < 481 GeV in the central dijet region.
Particle-level distributions of groomed AK4 width (charged-only) in 481 < PT < 614 GeV in the central dijet region.
Particle-level distributions of groomed AK4 width (charged-only) in 614 < PT < 800 GeV in the central dijet region.
Particle-level distributions of groomed AK4 width (charged-only) in 800 < PT < 1000 GeV in the central dijet region.
Particle-level distributions of groomed AK4 width (charged-only) in 1000 < PT < 4000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 width (charged-only) in 50 < PT < 65 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 width (charged-only) in 65 < PT < 88 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 width (charged-only) in 88 < PT < 120 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 width (charged-only) in 120 < PT < 150 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 width (charged-only) in 150 < PT < 186 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 width (charged-only) in 186 < PT < 254 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 width (charged-only) in 254 < PT < 326 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 width (charged-only) in 326 < PT < 408 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 width (charged-only) in 408 < PT < 481 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 width (charged-only) in 481 < PT < 614 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 width (charged-only) in 614 < PT < 800 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 width (charged-only) in 800 < PT < 1000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 width (charged-only) in 1000 < PT < 4000 GeV in the central dijet region.
Particle-level distributions of groomed AK4 width (charged-only) in 50 < PT < 65 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 width (charged-only) in 65 < PT < 88 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 width (charged-only) in 88 < PT < 120 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 width (charged-only) in 120 < PT < 150 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 width (charged-only) in 150 < PT < 186 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 width (charged-only) in 186 < PT < 254 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 width (charged-only) in 254 < PT < 326 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 width (charged-only) in 326 < PT < 408 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 width (charged-only) in 408 < PT < 481 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 width (charged-only) in 481 < PT < 614 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 width (charged-only) in 614 < PT < 800 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 width (charged-only) in 800 < PT < 1000 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 width (charged-only) in 1000 < PT < 4000 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 multiplicity in 50 < PT < 65 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 multiplicity in 65 < PT < 88 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 multiplicity in 88 < PT < 120 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 multiplicity in 120 < PT < 150 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 multiplicity in 150 < PT < 186 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 multiplicity in 186 < PT < 254 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 multiplicity in 254 < PT < 326 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 multiplicity in 326 < PT < 408 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 multiplicity in 408 < PT < 1500 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity in 50 < PT < 65 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity in 65 < PT < 88 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity in 88 < PT < 120 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity in 120 < PT < 150 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity in 150 < PT < 186 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity in 186 < PT < 254 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity in 254 < PT < 326 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity in 326 < PT < 408 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity in 408 < PT < 1500 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 multiplicity in 50 < PT < 65 GeV in the central dijet region.
Particle-level distributions of groomed AK4 multiplicity in 65 < PT < 88 GeV in the central dijet region.
Particle-level distributions of groomed AK4 multiplicity in 88 < PT < 120 GeV in the central dijet region.
Particle-level distributions of groomed AK4 multiplicity in 120 < PT < 150 GeV in the central dijet region.
Particle-level distributions of groomed AK4 multiplicity in 150 < PT < 186 GeV in the central dijet region.
Particle-level distributions of groomed AK4 multiplicity in 186 < PT < 254 GeV in the central dijet region.
Particle-level distributions of groomed AK4 multiplicity in 254 < PT < 326 GeV in the central dijet region.
Particle-level distributions of groomed AK4 multiplicity in 326 < PT < 408 GeV in the central dijet region.
Particle-level distributions of groomed AK4 multiplicity in 408 < PT < 481 GeV in the central dijet region.
Particle-level distributions of groomed AK4 multiplicity in 481 < PT < 614 GeV in the central dijet region.
Particle-level distributions of groomed AK4 multiplicity in 614 < PT < 800 GeV in the central dijet region.
Particle-level distributions of groomed AK4 multiplicity in 800 < PT < 1000 GeV in the central dijet region.
Particle-level distributions of groomed AK4 multiplicity in 1000 < PT < 4000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity in 50 < PT < 65 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity in 65 < PT < 88 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity in 88 < PT < 120 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity in 120 < PT < 150 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity in 150 < PT < 186 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity in 186 < PT < 254 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity in 254 < PT < 326 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity in 326 < PT < 408 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity in 408 < PT < 481 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity in 481 < PT < 614 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity in 614 < PT < 800 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity in 800 < PT < 1000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity in 1000 < PT < 4000 GeV in the central dijet region.
Particle-level distributions of groomed AK4 multiplicity in 50 < PT < 65 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 multiplicity in 65 < PT < 88 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 multiplicity in 88 < PT < 120 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 multiplicity in 120 < PT < 150 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 multiplicity in 150 < PT < 186 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 multiplicity in 186 < PT < 254 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 multiplicity in 254 < PT < 326 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 multiplicity in 326 < PT < 408 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 multiplicity in 408 < PT < 481 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 multiplicity in 481 < PT < 614 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 multiplicity in 614 < PT < 800 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 multiplicity in 800 < PT < 1000 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 multiplicity in 1000 < PT < 4000 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 pTD2 in 50 < PT < 65 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 pTD2 in 65 < PT < 88 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 pTD2 in 88 < PT < 120 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 pTD2 in 120 < PT < 150 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 pTD2 in 150 < PT < 186 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 pTD2 in 186 < PT < 254 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 pTD2 in 254 < PT < 326 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 pTD2 in 326 < PT < 408 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 pTD2 in 408 < PT < 1500 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 in 50 < PT < 65 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 in 65 < PT < 88 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 in 88 < PT < 120 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 in 120 < PT < 150 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 in 150 < PT < 186 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 in 186 < PT < 254 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 in 254 < PT < 326 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 in 326 < PT < 408 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 in 408 < PT < 1500 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 pTD2 in 50 < PT < 65 GeV in the central dijet region.
Particle-level distributions of groomed AK4 pTD2 in 65 < PT < 88 GeV in the central dijet region.
Particle-level distributions of groomed AK4 pTD2 in 88 < PT < 120 GeV in the central dijet region.
Particle-level distributions of groomed AK4 pTD2 in 120 < PT < 150 GeV in the central dijet region.
Particle-level distributions of groomed AK4 pTD2 in 150 < PT < 186 GeV in the central dijet region.
Particle-level distributions of groomed AK4 pTD2 in 186 < PT < 254 GeV in the central dijet region.
Particle-level distributions of groomed AK4 pTD2 in 254 < PT < 326 GeV in the central dijet region.
Particle-level distributions of groomed AK4 pTD2 in 326 < PT < 408 GeV in the central dijet region.
Particle-level distributions of groomed AK4 pTD2 in 408 < PT < 481 GeV in the central dijet region.
Particle-level distributions of groomed AK4 pTD2 in 481 < PT < 614 GeV in the central dijet region.
Particle-level distributions of groomed AK4 pTD2 in 614 < PT < 800 GeV in the central dijet region.
Particle-level distributions of groomed AK4 pTD2 in 800 < PT < 1000 GeV in the central dijet region.
Particle-level distributions of groomed AK4 pTD2 in 1000 < PT < 4000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 in 50 < PT < 65 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 in 65 < PT < 88 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 in 88 < PT < 120 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 in 120 < PT < 150 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 in 150 < PT < 186 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 in 186 < PT < 254 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 in 254 < PT < 326 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 in 326 < PT < 408 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 in 408 < PT < 481 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 in 481 < PT < 614 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 in 614 < PT < 800 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 in 800 < PT < 1000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 in 1000 < PT < 4000 GeV in the central dijet region.
Particle-level distributions of groomed AK4 pTD2 in 50 < PT < 65 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 pTD2 in 65 < PT < 88 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 pTD2 in 88 < PT < 120 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 pTD2 in 120 < PT < 150 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 pTD2 in 150 < PT < 186 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 pTD2 in 186 < PT < 254 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 pTD2 in 254 < PT < 326 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 pTD2 in 326 < PT < 408 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 pTD2 in 408 < PT < 481 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 pTD2 in 481 < PT < 614 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 pTD2 in 614 < PT < 800 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 pTD2 in 800 < PT < 1000 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 pTD2 in 1000 < PT < 4000 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 thrust in 50 < PT < 65 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 thrust in 65 < PT < 88 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 thrust in 88 < PT < 120 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 thrust in 120 < PT < 150 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 thrust in 150 < PT < 186 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 thrust in 186 < PT < 254 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 thrust in 254 < PT < 326 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 thrust in 326 < PT < 408 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 thrust in 408 < PT < 1500 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 thrust in 50 < PT < 65 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 thrust in 65 < PT < 88 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 thrust in 88 < PT < 120 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 thrust in 120 < PT < 150 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 thrust in 150 < PT < 186 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 thrust in 186 < PT < 254 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 thrust in 254 < PT < 326 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 thrust in 326 < PT < 408 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 thrust in 408 < PT < 1500 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 thrust in 50 < PT < 65 GeV in the central dijet region.
Particle-level distributions of groomed AK4 thrust in 65 < PT < 88 GeV in the central dijet region.
Particle-level distributions of groomed AK4 thrust in 88 < PT < 120 GeV in the central dijet region.
Particle-level distributions of groomed AK4 thrust in 120 < PT < 150 GeV in the central dijet region.
Particle-level distributions of groomed AK4 thrust in 150 < PT < 186 GeV in the central dijet region.
Particle-level distributions of groomed AK4 thrust in 186 < PT < 254 GeV in the central dijet region.
Particle-level distributions of groomed AK4 thrust in 254 < PT < 326 GeV in the central dijet region.
Particle-level distributions of groomed AK4 thrust in 326 < PT < 408 GeV in the central dijet region.
Particle-level distributions of groomed AK4 thrust in 408 < PT < 481 GeV in the central dijet region.
Particle-level distributions of groomed AK4 thrust in 481 < PT < 614 GeV in the central dijet region.
Particle-level distributions of groomed AK4 thrust in 614 < PT < 800 GeV in the central dijet region.
Particle-level distributions of groomed AK4 thrust in 800 < PT < 1000 GeV in the central dijet region.
Particle-level distributions of groomed AK4 thrust in 1000 < PT < 4000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 thrust in 50 < PT < 65 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 thrust in 65 < PT < 88 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 thrust in 88 < PT < 120 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 thrust in 120 < PT < 150 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 thrust in 150 < PT < 186 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 thrust in 186 < PT < 254 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 thrust in 254 < PT < 326 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 thrust in 326 < PT < 408 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 thrust in 408 < PT < 481 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 thrust in 481 < PT < 614 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 thrust in 614 < PT < 800 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 thrust in 800 < PT < 1000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 thrust in 1000 < PT < 4000 GeV in the central dijet region.
Particle-level distributions of groomed AK4 thrust in 50 < PT < 65 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 thrust in 65 < PT < 88 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 thrust in 88 < PT < 120 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 thrust in 120 < PT < 150 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 thrust in 150 < PT < 186 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 thrust in 186 < PT < 254 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 thrust in 254 < PT < 326 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 thrust in 326 < PT < 408 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 thrust in 408 < PT < 481 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 thrust in 481 < PT < 614 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 thrust in 614 < PT < 800 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 thrust in 800 < PT < 1000 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 thrust in 1000 < PT < 4000 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 width in 50 < PT < 65 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 width in 65 < PT < 88 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 width in 88 < PT < 120 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 width in 120 < PT < 150 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 width in 150 < PT < 186 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 width in 186 < PT < 254 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 width in 254 < PT < 326 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 width in 326 < PT < 408 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 width in 408 < PT < 1500 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 width in 50 < PT < 65 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 width in 65 < PT < 88 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 width in 88 < PT < 120 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 width in 120 < PT < 150 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 width in 150 < PT < 186 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 width in 186 < PT < 254 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 width in 254 < PT < 326 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 width in 326 < PT < 408 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 width in 408 < PT < 1500 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 width in 50 < PT < 65 GeV in the central dijet region.
Particle-level distributions of groomed AK4 width in 65 < PT < 88 GeV in the central dijet region.
Particle-level distributions of groomed AK4 width in 88 < PT < 120 GeV in the central dijet region.
Particle-level distributions of groomed AK4 width in 120 < PT < 150 GeV in the central dijet region.
Particle-level distributions of groomed AK4 width in 150 < PT < 186 GeV in the central dijet region.
Particle-level distributions of groomed AK4 width in 186 < PT < 254 GeV in the central dijet region.
Particle-level distributions of groomed AK4 width in 254 < PT < 326 GeV in the central dijet region.
Particle-level distributions of groomed AK4 width in 326 < PT < 408 GeV in the central dijet region.
Particle-level distributions of groomed AK4 width in 408 < PT < 481 GeV in the central dijet region.
Particle-level distributions of groomed AK4 width in 481 < PT < 614 GeV in the central dijet region.
Particle-level distributions of groomed AK4 width in 614 < PT < 800 GeV in the central dijet region.
Particle-level distributions of groomed AK4 width in 800 < PT < 1000 GeV in the central dijet region.
Particle-level distributions of groomed AK4 width in 1000 < PT < 4000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 width in 50 < PT < 65 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 width in 65 < PT < 88 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 width in 88 < PT < 120 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 width in 120 < PT < 150 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 width in 150 < PT < 186 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 width in 186 < PT < 254 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 width in 254 < PT < 326 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 width in 326 < PT < 408 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 width in 408 < PT < 481 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 width in 481 < PT < 614 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 width in 614 < PT < 800 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 width in 800 < PT < 1000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 width in 1000 < PT < 4000 GeV in the central dijet region.
Particle-level distributions of groomed AK4 width in 50 < PT < 65 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 width in 65 < PT < 88 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 width in 88 < PT < 120 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 width in 120 < PT < 150 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 width in 150 < PT < 186 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 width in 186 < PT < 254 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 width in 254 < PT < 326 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 width in 326 < PT < 408 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 width in 408 < PT < 481 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 width in 481 < PT < 614 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 width in 614 < PT < 800 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 width in 800 < PT < 1000 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 width in 1000 < PT < 4000 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 LHA in 50 < PT < 65 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 LHA in 65 < PT < 88 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 LHA in 88 < PT < 120 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 LHA in 150 < PT < 186 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 LHA in 186 < PT < 254 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 LHA in 254 < PT < 326 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 LHA in 326 < PT < 408 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 LHA in 408 < PT < 1500 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 LHA in 50 < PT < 65 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 LHA in 65 < PT < 88 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 LHA in 88 < PT < 120 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 LHA in 150 < PT < 186 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 LHA in 186 < PT < 254 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 LHA in 254 < PT < 326 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 LHA in 326 < PT < 408 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 LHA in 408 < PT < 481 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 LHA in 481 < PT < 614 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 LHA in 614 < PT < 800 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 LHA in 800 < PT < 1000 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 LHA in 1000 < PT < 4000 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 LHA in 50 < PT < 65 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 LHA in 65 < PT < 88 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 LHA in 88 < PT < 120 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 LHA in 120 < PT < 150 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 LHA in 150 < PT < 186 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 LHA in 186 < PT < 254 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 LHA in 254 < PT < 326 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 LHA in 326 < PT < 408 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 LHA in 408 < PT < 481 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 LHA in 481 < PT < 614 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 LHA in 614 < PT < 800 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 LHA in 800 < PT < 1000 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 LHA in 1000 < PT < 4000 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 LHA (charged-only) in 50 < PT < 65 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 LHA (charged-only) in 65 < PT < 88 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 LHA (charged-only) in 88 < PT < 120 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 LHA (charged-only) in 120 < PT < 150 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 LHA (charged-only) in 150 < PT < 186 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 LHA (charged-only) in 186 < PT < 254 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 LHA (charged-only) in 254 < PT < 326 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 LHA (charged-only) in 326 < PT < 408 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 LHA (charged-only) in 408 < PT < 1500 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 LHA (charged-only) in 50 < PT < 65 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 LHA (charged-only) in 65 < PT < 88 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 LHA (charged-only) in 88 < PT < 120 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 LHA (charged-only) in 120 < PT < 150 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 LHA (charged-only) in 150 < PT < 186 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 LHA (charged-only) in 186 < PT < 254 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 LHA (charged-only) in 254 < PT < 326 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 LHA (charged-only) in 326 < PT < 408 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 LHA (charged-only) in 408 < PT < 1500 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 LHA (charged-only) in 50 < PT < 65 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 LHA (charged-only) in 65 < PT < 88 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 LHA (charged-only) in 88 < PT < 120 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 LHA (charged-only) in 120 < PT < 150 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 LHA (charged-only) in 150 < PT < 186 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 LHA (charged-only) in 186 < PT < 254 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 LHA (charged-only) in 254 < PT < 326 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 LHA (charged-only) in 326 < PT < 408 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 LHA (charged-only) in 408 < PT < 481 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 LHA (charged-only) in 481 < PT < 614 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 LHA (charged-only) in 614 < PT < 800 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 LHA (charged-only) in 800 < PT < 1000 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 LHA (charged-only) in 1000 < PT < 4000 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 LHA (charged-only) in 50 < PT < 65 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 LHA (charged-only) in 65 < PT < 88 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 LHA (charged-only) in 88 < PT < 120 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 LHA (charged-only) in 120 < PT < 150 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 LHA (charged-only) in 150 < PT < 186 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 LHA (charged-only) in 186 < PT < 254 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 LHA (charged-only) in 254 < PT < 326 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 LHA (charged-only) in 326 < PT < 408 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 LHA (charged-only) in 408 < PT < 481 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 LHA (charged-only) in 481 < PT < 614 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 LHA (charged-only) in 614 < PT < 800 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 LHA (charged-only) in 800 < PT < 1000 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 LHA (charged-only) in 1000 < PT < 4000 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 multiplicity (charged-only) in 50 < PT < 65 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 multiplicity (charged-only) in 65 < PT < 88 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 multiplicity (charged-only) in 88 < PT < 120 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 multiplicity (charged-only) in 120 < PT < 150 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 multiplicity (charged-only) in 150 < PT < 186 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 multiplicity (charged-only) in 186 < PT < 254 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 multiplicity (charged-only) in 254 < PT < 326 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 multiplicity (charged-only) in 326 < PT < 408 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 multiplicity (charged-only) in 408 < PT < 1500 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 multiplicity (charged-only) in 50 < PT < 65 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 multiplicity (charged-only) in 65 < PT < 88 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 multiplicity (charged-only) in 88 < PT < 120 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 multiplicity (charged-only) in 120 < PT < 150 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 multiplicity (charged-only) in 150 < PT < 186 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 multiplicity (charged-only) in 186 < PT < 254 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 multiplicity (charged-only) in 254 < PT < 326 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 multiplicity (charged-only) in 326 < PT < 408 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 multiplicity (charged-only) in 408 < PT < 1500 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 multiplicity (charged-only) in 50 < PT < 65 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 multiplicity (charged-only) in 65 < PT < 88 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 multiplicity (charged-only) in 88 < PT < 120 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 multiplicity (charged-only) in 120 < PT < 150 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 multiplicity (charged-only) in 150 < PT < 186 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 multiplicity (charged-only) in 186 < PT < 254 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 multiplicity (charged-only) in 254 < PT < 326 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 multiplicity (charged-only) in 326 < PT < 408 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 multiplicity (charged-only) in 408 < PT < 481 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 multiplicity (charged-only) in 481 < PT < 614 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 multiplicity (charged-only) in 614 < PT < 800 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 multiplicity (charged-only) in 800 < PT < 1000 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 multiplicity (charged-only) in 1000 < PT < 4000 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 multiplicity (charged-only) in 50 < PT < 65 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 multiplicity (charged-only) in 65 < PT < 88 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 multiplicity (charged-only) in 88 < PT < 120 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 multiplicity (charged-only) in 120 < PT < 150 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 multiplicity (charged-only) in 150 < PT < 186 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 multiplicity (charged-only) in 186 < PT < 254 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 multiplicity (charged-only) in 254 < PT < 326 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 multiplicity (charged-only) in 326 < PT < 408 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 multiplicity (charged-only) in 408 < PT < 481 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 multiplicity (charged-only) in 481 < PT < 614 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 multiplicity (charged-only) in 614 < PT < 800 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 multiplicity (charged-only) in 800 < PT < 1000 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 multiplicity (charged-only) in 1000 < PT < 4000 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 pTD2 (charged-only) in 50 < PT < 65 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 pTD2 (charged-only) in 65 < PT < 88 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 pTD2 (charged-only) in 88 < PT < 120 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 pTD2 (charged-only) in 120 < PT < 150 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 pTD2 (charged-only) in 150 < PT < 186 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 pTD2 (charged-only) in 186 < PT < 254 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 pTD2 (charged-only) in 254 < PT < 326 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 pTD2 (charged-only) in 326 < PT < 408 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 pTD2 (charged-only) in 408 < PT < 1500 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 pTD2 (charged-only) in 50 < PT < 65 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 pTD2 (charged-only) in 65 < PT < 88 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 pTD2 (charged-only) in 88 < PT < 120 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 pTD2 (charged-only) in 120 < PT < 150 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 pTD2 (charged-only) in 150 < PT < 186 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 pTD2 (charged-only) in 186 < PT < 254 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 pTD2 (charged-only) in 254 < PT < 326 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 pTD2 (charged-only) in 326 < PT < 408 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 pTD2 (charged-only) in 408 < PT < 1500 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 pTD2 (charged-only) in 50 < PT < 65 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 pTD2 (charged-only) in 65 < PT < 88 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 pTD2 (charged-only) in 88 < PT < 120 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 pTD2 (charged-only) in 120 < PT < 150 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 pTD2 (charged-only) in 150 < PT < 186 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 pTD2 (charged-only) in 186 < PT < 254 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 pTD2 (charged-only) in 254 < PT < 326 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 pTD2 (charged-only) in 326 < PT < 408 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 pTD2 (charged-only) in 408 < PT < 481 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 pTD2 (charged-only) in 481 < PT < 614 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 pTD2 (charged-only) in 614 < PT < 800 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 pTD2 (charged-only) in 800 < PT < 1000 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 pTD2 (charged-only) in 1000 < PT < 4000 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 pTD2 (charged-only) in 50 < PT < 65 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 pTD2 (charged-only) in 65 < PT < 88 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 pTD2 (charged-only) in 88 < PT < 120 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 pTD2 (charged-only) in 120 < PT < 150 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 pTD2 (charged-only) in 150 < PT < 186 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 pTD2 (charged-only) in 186 < PT < 254 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 pTD2 (charged-only) in 254 < PT < 326 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 pTD2 (charged-only) in 326 < PT < 408 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 pTD2 (charged-only) in 408 < PT < 481 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 pTD2 (charged-only) in 481 < PT < 614 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 pTD2 (charged-only) in 614 < PT < 800 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 pTD2 (charged-only) in 800 < PT < 1000 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 pTD2 (charged-only) in 1000 < PT < 4000 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 thrust (charged-only) in 50 < PT < 65 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 thrust (charged-only) in 65 < PT < 88 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 thrust (charged-only) in 88 < PT < 120 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 thrust (charged-only) in 120 < PT < 150 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 thrust (charged-only) in 150 < PT < 186 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 thrust (charged-only) in 186 < PT < 254 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 thrust (charged-only) in 254 < PT < 326 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 thrust (charged-only) in 326 < PT < 408 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 thrust (charged-only) in 408 < PT < 1500 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 thrust (charged-only) in 50 < PT < 65 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 thrust (charged-only) in 65 < PT < 88 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 thrust (charged-only) in 88 < PT < 120 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 thrust (charged-only) in 120 < PT < 150 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 thrust (charged-only) in 150 < PT < 186 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 thrust (charged-only) in 186 < PT < 254 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 thrust (charged-only) in 254 < PT < 326 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 thrust (charged-only) in 326 < PT < 408 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 thrust (charged-only) in 408 < PT < 1500 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 thrust (charged-only) in 50 < PT < 65 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 thrust (charged-only) in 65 < PT < 88 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 thrust (charged-only) in 88 < PT < 120 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 thrust (charged-only) in 120 < PT < 150 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 thrust (charged-only) in 150 < PT < 186 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 thrust (charged-only) in 186 < PT < 254 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 thrust (charged-only) in 254 < PT < 326 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 thrust (charged-only) in 326 < PT < 408 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 thrust (charged-only) in 408 < PT < 481 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 thrust (charged-only) in 481 < PT < 614 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 thrust (charged-only) in 614 < PT < 800 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 thrust (charged-only) in 800 < PT < 1000 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 thrust (charged-only) in 1000 < PT < 4000 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 thrust (charged-only) in 50 < PT < 65 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 thrust (charged-only) in 65 < PT < 88 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 thrust (charged-only) in 88 < PT < 120 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 thrust (charged-only) in 120 < PT < 150 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 thrust (charged-only) in 150 < PT < 186 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 thrust (charged-only) in 186 < PT < 254 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 thrust (charged-only) in 254 < PT < 326 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 thrust (charged-only) in 326 < PT < 408 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 thrust (charged-only) in 408 < PT < 481 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 thrust (charged-only) in 481 < PT < 614 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 thrust (charged-only) in 614 < PT < 800 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 thrust (charged-only) in 800 < PT < 1000 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 thrust (charged-only) in 1000 < PT < 4000 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 width (charged-only) in 50 < PT < 65 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 width (charged-only) in 65 < PT < 88 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 width (charged-only) in 88 < PT < 120 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 width (charged-only) in 120 < PT < 150 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 width (charged-only) in 150 < PT < 186 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 width (charged-only) in 186 < PT < 254 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 width (charged-only) in 254 < PT < 326 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 width (charged-only) in 326 < PT < 408 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 width (charged-only) in 408 < PT < 1500 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 width (charged-only) in 50 < PT < 65 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 width (charged-only) in 65 < PT < 88 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 width (charged-only) in 88 < PT < 120 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 width (charged-only) in 120 < PT < 150 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 width (charged-only) in 150 < PT < 186 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 width (charged-only) in 186 < PT < 254 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 width (charged-only) in 254 < PT < 326 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 width (charged-only) in 326 < PT < 408 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 width (charged-only) in 408 < PT < 1500 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 width (charged-only) in 50 < PT < 65 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 width (charged-only) in 65 < PT < 88 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 width (charged-only) in 88 < PT < 120 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 width (charged-only) in 120 < PT < 150 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 width (charged-only) in 150 < PT < 186 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 width (charged-only) in 186 < PT < 254 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 width (charged-only) in 254 < PT < 326 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 width (charged-only) in 326 < PT < 408 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 width (charged-only) in 408 < PT < 481 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 width (charged-only) in 481 < PT < 614 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 width (charged-only) in 614 < PT < 800 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 width (charged-only) in 800 < PT < 1000 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 width (charged-only) in 1000 < PT < 4000 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 width (charged-only) in 50 < PT < 65 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 width (charged-only) in 65 < PT < 88 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 width (charged-only) in 88 < PT < 120 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 width (charged-only) in 120 < PT < 150 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 width (charged-only) in 150 < PT < 186 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 width (charged-only) in 186 < PT < 254 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 width (charged-only) in 254 < PT < 326 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 width (charged-only) in 326 < PT < 408 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 width (charged-only) in 408 < PT < 481 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 width (charged-only) in 481 < PT < 614 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 width (charged-only) in 614 < PT < 800 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 width (charged-only) in 800 < PT < 1000 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 width (charged-only) in 1000 < PT < 4000 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 multiplicity in 50 < PT < 65 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 multiplicity in 65 < PT < 88 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 multiplicity in 88 < PT < 120 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 multiplicity in 120 < PT < 150 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 multiplicity in 150 < PT < 186 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 multiplicity in 186 < PT < 254 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 multiplicity in 254 < PT < 326 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 multiplicity in 326 < PT < 408 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 multiplicity in 408 < PT < 1500 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 multiplicity in 50 < PT < 65 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 multiplicity in 65 < PT < 88 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 multiplicity in 88 < PT < 120 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 multiplicity in 120 < PT < 150 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 multiplicity in 150 < PT < 186 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 multiplicity in 186 < PT < 254 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 multiplicity in 254 < PT < 326 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 multiplicity in 326 < PT < 408 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 multiplicity in 408 < PT < 481 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 multiplicity in 481 < PT < 614 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 multiplicity in 614 < PT < 800 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 multiplicity in 800 < PT < 1000 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 multiplicity in 1000 < PT < 4000 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 multiplicity in 50 < PT < 65 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 multiplicity in 65 < PT < 88 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 multiplicity in 88 < PT < 120 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 multiplicity in 120 < PT < 150 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 multiplicity in 150 < PT < 186 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 multiplicity in 186 < PT < 254 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 multiplicity in 254 < PT < 326 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 multiplicity in 326 < PT < 408 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 multiplicity in 408 < PT < 481 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 multiplicity in 481 < PT < 614 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 multiplicity in 614 < PT < 800 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 multiplicity in 800 < PT < 1000 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 multiplicity in 1000 < PT < 4000 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 pTD2 in 50 < PT < 65 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 pTD2 in 65 < PT < 88 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 pTD2 in 88 < PT < 120 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 pTD2 in 120 < PT < 150 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 pTD2 in 150 < PT < 186 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 pTD2 in 186 < PT < 254 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 pTD2 in 254 < PT < 326 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 pTD2 in 326 < PT < 408 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 pTD2 in 408 < PT < 1500 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 pTD2 in 50 < PT < 65 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 pTD2 in 65 < PT < 88 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 pTD2 in 88 < PT < 120 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 pTD2 in 120 < PT < 150 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 pTD2 in 150 < PT < 186 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 pTD2 in 186 < PT < 254 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 pTD2 in 254 < PT < 326 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 pTD2 in 326 < PT < 408 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 pTD2 in 408 < PT < 481 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 pTD2 in 481 < PT < 614 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 pTD2 in 614 < PT < 800 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 pTD2 in 800 < PT < 1000 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 pTD2 in 1000 < PT < 4000 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 pTD2 in 50 < PT < 65 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 pTD2 in 65 < PT < 88 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 pTD2 in 88 < PT < 120 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 pTD2 in 120 < PT < 150 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 pTD2 in 150 < PT < 186 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 pTD2 in 186 < PT < 254 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 pTD2 in 254 < PT < 326 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 pTD2 in 326 < PT < 408 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 pTD2 in 408 < PT < 481 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 pTD2 in 481 < PT < 614 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 pTD2 in 614 < PT < 800 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 pTD2 in 800 < PT < 1000 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 pTD2 in 1000 < PT < 4000 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 thrust in 50 < PT < 65 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 thrust in 65 < PT < 88 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 thrust in 88 < PT < 120 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 thrust in 120 < PT < 150 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 thrust in 150 < PT < 186 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 thrust in 186 < PT < 254 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 thrust in 254 < PT < 326 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 thrust in 326 < PT < 408 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 thrust in 408 < PT < 1500 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 thrust in 50 < PT < 65 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 thrust in 65 < PT < 88 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 thrust in 88 < PT < 120 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 thrust in 120 < PT < 150 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 thrust in 150 < PT < 186 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 thrust in 186 < PT < 254 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 thrust in 254 < PT < 326 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 thrust in 326 < PT < 408 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 thrust in 408 < PT < 481 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 thrust in 481 < PT < 614 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 thrust in 614 < PT < 800 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 thrust in 800 < PT < 1000 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 thrust in 1000 < PT < 4000 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 thrust in 50 < PT < 65 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 thrust in 65 < PT < 88 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 thrust in 88 < PT < 120 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 thrust in 120 < PT < 150 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 thrust in 150 < PT < 186 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 thrust in 186 < PT < 254 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 thrust in 254 < PT < 326 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 thrust in 326 < PT < 408 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 thrust in 408 < PT < 481 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 thrust in 481 < PT < 614 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 thrust in 614 < PT < 800 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 thrust in 800 < PT < 1000 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 thrust in 1000 < PT < 4000 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 width in 50 < PT < 65 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 width in 65 < PT < 88 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 width in 88 < PT < 120 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 width in 120 < PT < 150 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 width in 150 < PT < 186 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 width in 186 < PT < 254 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 width in 254 < PT < 326 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 width in 326 < PT < 408 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 width in 408 < PT < 1500 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 width in 50 < PT < 65 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 width in 65 < PT < 88 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 width in 88 < PT < 120 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 width in 120 < PT < 150 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 width in 150 < PT < 186 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 width in 186 < PT < 254 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 width in 254 < PT < 326 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 width in 326 < PT < 408 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 width in 408 < PT < 481 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 width in 481 < PT < 614 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 width in 614 < PT < 800 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 width in 800 < PT < 1000 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 width in 1000 < PT < 4000 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 width in 50 < PT < 65 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 width in 65 < PT < 88 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 width in 88 < PT < 120 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 width in 120 < PT < 150 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 width in 150 < PT < 186 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 width in 186 < PT < 254 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 width in 254 < PT < 326 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 width in 326 < PT < 408 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 width in 408 < PT < 481 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 width in 481 < PT < 614 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 width in 614 < PT < 800 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 width in 800 < PT < 1000 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 width in 1000 < PT < 4000 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 LHA in 50 < PT < 65 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 LHA in 65 < PT < 88 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 LHA in 88 < PT < 120 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 LHA in 120 < PT < 150 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 LHA in 150 < PT < 186 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 LHA in 186 < PT < 254 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 LHA in 254 < PT < 326 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 LHA in 326 < PT < 408 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 LHA in 408 < PT < 1500 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 LHA in 50 < PT < 65 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 LHA in 65 < PT < 88 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 LHA in 88 < PT < 120 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 LHA in 120 < PT < 150 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 LHA in 150 < PT < 186 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 LHA in 186 < PT < 254 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 LHA in 254 < PT < 326 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 LHA in 326 < PT < 408 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 LHA in 408 < PT < 1500 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 LHA in 50 < PT < 65 GeV in the central dijet region.
Particle-level distributions of groomed AK8 LHA in 65 < PT < 88 GeV in the central dijet region.
Particle-level distributions of groomed AK8 LHA in 88 < PT < 120 GeV in the central dijet region.
Particle-level distributions of groomed AK8 LHA in 120 < PT < 150 GeV in the central dijet region.
Particle-level distributions of groomed AK8 LHA in 150 < PT < 186 GeV in the central dijet region.
Particle-level distributions of groomed AK8 LHA in 186 < PT < 254 GeV in the central dijet region.
Particle-level distributions of groomed AK8 LHA in 254 < PT < 326 GeV in the central dijet region.
Particle-level distributions of groomed AK8 LHA in 326 < PT < 408 GeV in the central dijet region.
Particle-level distributions of groomed AK8 LHA in 408 < PT < 481 GeV in the central dijet region.
Particle-level distributions of groomed AK8 LHA in 481 < PT < 614 GeV in the central dijet region.
Particle-level distributions of groomed AK8 LHA in 614 < PT < 800 GeV in the central dijet region.
Particle-level distributions of groomed AK8 LHA in 800 < PT < 1000 GeV in the central dijet region.
Particle-level distributions of groomed AK8 LHA in 1000 < PT < 4000 GeV in the central dijet region.
Particle-level distributions of groomed AK8 LHA in 50 < PT < 65 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 LHA in 65 < PT < 88 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 LHA in 88 < PT < 120 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 LHA in 120 < PT < 150 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 LHA in 150 < PT < 186 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 LHA in 186 < PT < 254 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 LHA in 254 < PT < 326 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 LHA in 326 < PT < 408 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 LHA in 408 < PT < 481 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 LHA in 481 < PT < 614 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 LHA in 614 < PT < 800 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 LHA in 800 < PT < 1000 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 LHA in 1000 < PT < 4000 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 LHA (charged-only) in 50 < PT < 65 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 LHA (charged-only) in 65 < PT < 88 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 LHA (charged-only) in 88 < PT < 120 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 LHA (charged-only) in 120 < PT < 150 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 LHA (charged-only) in 150 < PT < 186 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 LHA (charged-only) in 186 < PT < 254 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 LHA (charged-only) in 254 < PT < 326 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 LHA (charged-only) in 326 < PT < 408 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 LHA (charged-only) in 408 < PT < 1500 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 LHA (charged-only) in 50 < PT < 65 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 LHA (charged-only) in 65 < PT < 88 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 LHA (charged-only) in 88 < PT < 120 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 LHA (charged-only) in 120 < PT < 150 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 LHA (charged-only) in 150 < PT < 186 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 LHA (charged-only) in 186 < PT < 254 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 LHA (charged-only) in 254 < PT < 326 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 LHA (charged-only) in 326 < PT < 408 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 LHA (charged-only) in 408 < PT < 1500 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 LHA (charged-only) in 50 < PT < 65 GeV in the central dijet region.
Particle-level distributions of groomed AK8 LHA (charged-only) in 65 < PT < 88 GeV in the central dijet region.
Particle-level distributions of groomed AK8 LHA (charged-only) in 88 < PT < 120 GeV in the central dijet region.
Particle-level distributions of groomed AK8 LHA (charged-only) in 120 < PT < 150 GeV in the central dijet region.
Particle-level distributions of groomed AK8 LHA (charged-only) in 150 < PT < 186 GeV in the central dijet region.
Particle-level distributions of groomed AK8 LHA (charged-only) in 186 < PT < 254 GeV in the central dijet region.
Particle-level distributions of groomed AK8 LHA (charged-only) in 254 < PT < 326 GeV in the central dijet region.
Particle-level distributions of groomed AK8 LHA (charged-only) in 326 < PT < 408 GeV in the central dijet region.
Particle-level distributions of groomed AK8 LHA (charged-only) in 408 < PT < 481 GeV in the central dijet region.
Particle-level distributions of groomed AK8 LHA (charged-only) in 481 < PT < 614 GeV in the central dijet region.
Particle-level distributions of groomed AK8 LHA (charged-only) in 614 < PT < 800 GeV in the central dijet region.
Particle-level distributions of groomed AK8 LHA (charged-only) in 800 < PT < 1000 GeV in the central dijet region.
Particle-level distributions of groomed AK8 LHA (charged-only) in 1000 < PT < 4000 GeV in the central dijet region.
Particle-level distributions of groomed AK8 LHA (charged-only) in 50 < PT < 65 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 LHA (charged-only) in 65 < PT < 88 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 LHA (charged-only) in 88 < PT < 120 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 LHA (charged-only) in 120 < PT < 150 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 LHA (charged-only) in 150 < PT < 186 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 LHA (charged-only) in 186 < PT < 254 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 LHA (charged-only) in 254 < PT < 326 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 LHA (charged-only) in 326 < PT < 408 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 LHA (charged-only) in 408 < PT < 481 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 LHA (charged-only) in 481 < PT < 614 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 LHA (charged-only) in 614 < PT < 800 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 LHA (charged-only) in 800 < PT < 1000 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 LHA (charged-only) in 1000 < PT < 4000 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 multiplicity (charged-only) in 50 < PT < 65 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 multiplicity (charged-only) in 65 < PT < 88 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 multiplicity (charged-only) in 88 < PT < 120 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 multiplicity (charged-only) in 120 < PT < 150 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 multiplicity (charged-only) in 150 < PT < 186 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 multiplicity (charged-only) in 186 < PT < 254 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 multiplicity (charged-only) in 254 < PT < 326 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 multiplicity (charged-only) in 326 < PT < 408 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 multiplicity (charged-only) in 408 < PT < 1500 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 multiplicity (charged-only) in 50 < PT < 65 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 multiplicity (charged-only) in 65 < PT < 88 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 multiplicity (charged-only) in 88 < PT < 120 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 multiplicity (charged-only) in 120 < PT < 150 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 multiplicity (charged-only) in 150 < PT < 186 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 multiplicity (charged-only) in 186 < PT < 254 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 multiplicity (charged-only) in 254 < PT < 326 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 multiplicity (charged-only) in 326 < PT < 408 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 multiplicity (charged-only) in 408 < PT < 1500 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 multiplicity (charged-only) in 50 < PT < 65 GeV in the central dijet region.
Particle-level distributions of groomed AK8 multiplicity (charged-only) in 65 < PT < 88 GeV in the central dijet region.
Particle-level distributions of groomed AK8 multiplicity (charged-only) in 88 < PT < 120 GeV in the central dijet region.
Particle-level distributions of groomed AK8 multiplicity (charged-only) in 120 < PT < 150 GeV in the central dijet region.
Particle-level distributions of groomed AK8 multiplicity (charged-only) in 150 < PT < 186 GeV in the central dijet region.
Particle-level distributions of groomed AK8 multiplicity (charged-only) in 186 < PT < 254 GeV in the central dijet region.
Particle-level distributions of groomed AK8 multiplicity (charged-only) in 254 < PT < 326 GeV in the central dijet region.
Particle-level distributions of groomed AK8 multiplicity (charged-only) in 326 < PT < 408 GeV in the central dijet region.
Particle-level distributions of groomed AK8 multiplicity (charged-only) in 408 < PT < 481 GeV in the central dijet region.
Particle-level distributions of groomed AK8 multiplicity (charged-only) in 481 < PT < 614 GeV in the central dijet region.
Particle-level distributions of groomed AK8 multiplicity (charged-only) in 614 < PT < 800 GeV in the central dijet region.
Particle-level distributions of groomed AK8 multiplicity (charged-only) in 800 < PT < 1000 GeV in the central dijet region.
Particle-level distributions of groomed AK8 multiplicity (charged-only) in 1000 < PT < 4000 GeV in the central dijet region.
Particle-level distributions of groomed AK8 multiplicity (charged-only) in 50 < PT < 65 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 multiplicity (charged-only) in 65 < PT < 88 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 multiplicity (charged-only) in 88 < PT < 120 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 multiplicity (charged-only) in 120 < PT < 150 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 multiplicity (charged-only) in 150 < PT < 186 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 multiplicity (charged-only) in 186 < PT < 254 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 multiplicity (charged-only) in 254 < PT < 326 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 multiplicity (charged-only) in 326 < PT < 408 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 multiplicity (charged-only) in 408 < PT < 481 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 multiplicity (charged-only) in 481 < PT < 614 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 multiplicity (charged-only) in 614 < PT < 800 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 multiplicity (charged-only) in 800 < PT < 1000 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 multiplicity (charged-only) in 1000 < PT < 4000 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 pTD2 (charged-only) in 50 < PT < 65 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 pTD2 (charged-only) in 65 < PT < 88 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 pTD2 (charged-only) in 88 < PT < 120 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 pTD2 (charged-only) in 120 < PT < 150 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 pTD2 (charged-only) in 150 < PT < 186 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 pTD2 (charged-only) in 186 < PT < 254 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 pTD2 (charged-only) in 254 < PT < 326 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 pTD2 (charged-only) in 326 < PT < 408 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 pTD2 (charged-only) in 408 < PT < 1500 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 pTD2 (charged-only) in 50 < PT < 65 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 pTD2 (charged-only) in 65 < PT < 88 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 pTD2 (charged-only) in 88 < PT < 120 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 pTD2 (charged-only) in 120 < PT < 150 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 pTD2 (charged-only) in 150 < PT < 186 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 pTD2 (charged-only) in 186 < PT < 254 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 pTD2 (charged-only) in 254 < PT < 326 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 pTD2 (charged-only) in 326 < PT < 408 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 pTD2 (charged-only) in 408 < PT < 1500 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 pTD2 (charged-only) in 50 < PT < 65 GeV in the central dijet region.
Particle-level distributions of groomed AK8 pTD2 (charged-only) in 65 < PT < 88 GeV in the central dijet region.
Particle-level distributions of groomed AK8 pTD2 (charged-only) in 88 < PT < 120 GeV in the central dijet region.
Particle-level distributions of groomed AK8 pTD2 (charged-only) in 120 < PT < 150 GeV in the central dijet region.
Particle-level distributions of groomed AK8 pTD2 (charged-only) in 150 < PT < 186 GeV in the central dijet region.
Particle-level distributions of groomed AK8 pTD2 (charged-only) in 186 < PT < 254 GeV in the central dijet region.
Particle-level distributions of groomed AK8 pTD2 (charged-only) in 254 < PT < 326 GeV in the central dijet region.
Particle-level distributions of groomed AK8 pTD2 (charged-only) in 326 < PT < 408 GeV in the central dijet region.
Particle-level distributions of groomed AK8 pTD2 (charged-only) in 408 < PT < 481 GeV in the central dijet region.
Particle-level distributions of groomed AK8 pTD2 (charged-only) in 481 < PT < 614 GeV in the central dijet region.
Particle-level distributions of groomed AK8 pTD2 (charged-only) in 614 < PT < 800 GeV in the central dijet region.
Particle-level distributions of groomed AK8 pTD2 (charged-only) in 800 < PT < 1000 GeV in the central dijet region.
Particle-level distributions of groomed AK8 pTD2 (charged-only) in 1000 < PT < 4000 GeV in the central dijet region.
Particle-level distributions of groomed AK8 pTD2 (charged-only) in 50 < PT < 65 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 pTD2 (charged-only) in 65 < PT < 88 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 pTD2 (charged-only) in 88 < PT < 120 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 pTD2 (charged-only) in 120 < PT < 150 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 pTD2 (charged-only) in 150 < PT < 186 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 pTD2 (charged-only) in 186 < PT < 254 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 pTD2 (charged-only) in 254 < PT < 326 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 pTD2 (charged-only) in 326 < PT < 408 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 pTD2 (charged-only) in 408 < PT < 481 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 pTD2 (charged-only) in 481 < PT < 614 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 pTD2 (charged-only) in 614 < PT < 800 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 pTD2 (charged-only) in 800 < PT < 1000 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 pTD2 (charged-only) in 1000 < PT < 4000 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 thrust (charged-only) in 50 < PT < 65 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 thrust (charged-only) in 65 < PT < 88 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 thrust (charged-only) in 88 < PT < 120 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 thrust (charged-only) in 120 < PT < 150 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 thrust (charged-only) in 150 < PT < 186 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 thrust (charged-only) in 186 < PT < 254 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 thrust (charged-only) in 254 < PT < 326 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 thrust (charged-only) in 326 < PT < 408 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 thrust (charged-only) in 408 < PT < 1500 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 thrust (charged-only) in 50 < PT < 65 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 thrust (charged-only) in 65 < PT < 88 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 thrust (charged-only) in 88 < PT < 120 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 thrust (charged-only) in 120 < PT < 150 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 thrust (charged-only) in 150 < PT < 186 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 thrust (charged-only) in 186 < PT < 254 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 thrust (charged-only) in 254 < PT < 326 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 thrust (charged-only) in 326 < PT < 408 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 thrust (charged-only) in 408 < PT < 1500 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 thrust (charged-only) in 50 < PT < 65 GeV in the central dijet region.
Particle-level distributions of groomed AK8 thrust (charged-only) in 65 < PT < 88 GeV in the central dijet region.
Particle-level distributions of groomed AK8 thrust (charged-only) in 88 < PT < 120 GeV in the central dijet region.
Particle-level distributions of groomed AK8 thrust (charged-only) in 120 < PT < 150 GeV in the central dijet region.
Particle-level distributions of groomed AK8 thrust (charged-only) in 150 < PT < 186 GeV in the central dijet region.
Particle-level distributions of groomed AK8 thrust (charged-only) in 186 < PT < 254 GeV in the central dijet region.
Particle-level distributions of groomed AK8 thrust (charged-only) in 254 < PT < 326 GeV in the central dijet region.
Particle-level distributions of groomed AK8 thrust (charged-only) in 326 < PT < 408 GeV in the central dijet region.
Particle-level distributions of groomed AK8 thrust (charged-only) in 408 < PT < 481 GeV in the central dijet region.
Particle-level distributions of groomed AK8 thrust (charged-only) in 481 < PT < 614 GeV in the central dijet region.
Particle-level distributions of groomed AK8 thrust (charged-only) in 614 < PT < 800 GeV in the central dijet region.
Particle-level distributions of groomed AK8 thrust (charged-only) in 800 < PT < 1000 GeV in the central dijet region.
Particle-level distributions of groomed AK8 thrust (charged-only) in 1000 < PT < 4000 GeV in the central dijet region.
Particle-level distributions of groomed AK8 thrust (charged-only) in 50 < PT < 65 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 thrust (charged-only) in 65 < PT < 88 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 thrust (charged-only) in 88 < PT < 120 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 thrust (charged-only) in 120 < PT < 150 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 thrust (charged-only) in 150 < PT < 186 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 thrust (charged-only) in 186 < PT < 254 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 thrust (charged-only) in 254 < PT < 326 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 thrust (charged-only) in 326 < PT < 408 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 thrust (charged-only) in 408 < PT < 481 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 thrust (charged-only) in 481 < PT < 614 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 thrust (charged-only) in 614 < PT < 800 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 thrust (charged-only) in 800 < PT < 1000 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 thrust (charged-only) in 1000 < PT < 4000 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 width (charged-only) in 50 < PT < 65 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 width (charged-only) in 65 < PT < 88 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 width (charged-only) in 88 < PT < 120 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 width (charged-only) in 120 < PT < 150 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 width (charged-only) in 150 < PT < 186 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 width (charged-only) in 186 < PT < 254 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 width (charged-only) in 254 < PT < 326 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 width (charged-only) in 326 < PT < 408 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 width (charged-only) in 408 < PT < 1500 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 width (charged-only) in 50 < PT < 65 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 width (charged-only) in 65 < PT < 88 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 width (charged-only) in 88 < PT < 120 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 width (charged-only) in 120 < PT < 150 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 width (charged-only) in 150 < PT < 186 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 width (charged-only) in 186 < PT < 254 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 width (charged-only) in 254 < PT < 326 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 width (charged-only) in 326 < PT < 408 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 width (charged-only) in 408 < PT < 1500 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 width (charged-only) in 50 < PT < 65 GeV in the central dijet region.
Particle-level distributions of groomed AK8 width (charged-only) in 65 < PT < 88 GeV in the central dijet region.
Particle-level distributions of groomed AK8 width (charged-only) in 88 < PT < 120 GeV in the central dijet region.
Particle-level distributions of groomed AK8 width (charged-only) in 120 < PT < 150 GeV in the central dijet region.
Particle-level distributions of groomed AK8 width (charged-only) in 150 < PT < 186 GeV in the central dijet region.
Particle-level distributions of groomed AK8 width (charged-only) in 186 < PT < 254 GeV in the central dijet region.
Particle-level distributions of groomed AK8 width (charged-only) in 254 < PT < 326 GeV in the central dijet region.
Particle-level distributions of groomed AK8 width (charged-only) in 326 < PT < 408 GeV in the central dijet region.
Particle-level distributions of groomed AK8 width (charged-only) in 408 < PT < 481 GeV in the central dijet region.
Particle-level distributions of groomed AK8 width (charged-only) in 481 < PT < 614 GeV in the central dijet region.
Particle-level distributions of groomed AK8 width (charged-only) in 614 < PT < 800 GeV in the central dijet region.
Particle-level distributions of groomed AK8 width (charged-only) in 800 < PT < 1000 GeV in the central dijet region.
Particle-level distributions of groomed AK8 width (charged-only) in 1000 < PT < 4000 GeV in the central dijet region.
Particle-level distributions of groomed AK8 width (charged-only) in 50 < PT < 65 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 width (charged-only) in 65 < PT < 88 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 width (charged-only) in 88 < PT < 120 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 width (charged-only) in 120 < PT < 150 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 width (charged-only) in 150 < PT < 186 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 width (charged-only) in 186 < PT < 254 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 width (charged-only) in 254 < PT < 326 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 width (charged-only) in 326 < PT < 408 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 width (charged-only) in 408 < PT < 481 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 width (charged-only) in 481 < PT < 614 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 width (charged-only) in 614 < PT < 800 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 width (charged-only) in 800 < PT < 1000 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 width (charged-only) in 1000 < PT < 4000 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 multiplicity in 50 < PT < 65 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 multiplicity in 65 < PT < 88 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 multiplicity in 88 < PT < 120 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 multiplicity in 120 < PT < 150 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 multiplicity in 150 < PT < 186 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 multiplicity in 186 < PT < 254 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 multiplicity in 254 < PT < 326 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 multiplicity in 326 < PT < 408 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 multiplicity in 408 < PT < 1500 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 multiplicity in 50 < PT < 65 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 multiplicity in 65 < PT < 88 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 multiplicity in 88 < PT < 120 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 multiplicity in 120 < PT < 150 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 multiplicity in 150 < PT < 186 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 multiplicity in 186 < PT < 254 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 multiplicity in 254 < PT < 326 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 multiplicity in 326 < PT < 408 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 multiplicity in 408 < PT < 1500 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 multiplicity in 50 < PT < 65 GeV in the central dijet region.
Particle-level distributions of groomed AK8 multiplicity in 65 < PT < 88 GeV in the central dijet region.
Particle-level distributions of groomed AK8 multiplicity in 88 < PT < 120 GeV in the central dijet region.
Particle-level distributions of groomed AK8 multiplicity in 120 < PT < 150 GeV in the central dijet region.
Particle-level distributions of groomed AK8 multiplicity in 150 < PT < 186 GeV in the central dijet region.
Particle-level distributions of groomed AK8 multiplicity in 186 < PT < 254 GeV in the central dijet region.
Particle-level distributions of groomed AK8 multiplicity in 254 < PT < 326 GeV in the central dijet region.
Particle-level distributions of groomed AK8 multiplicity in 326 < PT < 408 GeV in the central dijet region.
Particle-level distributions of groomed AK8 multiplicity in 408 < PT < 481 GeV in the central dijet region.
Particle-level distributions of groomed AK8 multiplicity in 481 < PT < 614 GeV in the central dijet region.
Particle-level distributions of groomed AK8 multiplicity in 614 < PT < 800 GeV in the central dijet region.
Particle-level distributions of groomed AK8 multiplicity in 800 < PT < 1000 GeV in the central dijet region.
Particle-level distributions of groomed AK8 multiplicity in 1000 < PT < 4000 GeV in the central dijet region.
Particle-level distributions of groomed AK8 multiplicity in 50 < PT < 65 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 multiplicity in 65 < PT < 88 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 multiplicity in 88 < PT < 120 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 multiplicity in 120 < PT < 150 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 multiplicity in 150 < PT < 186 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 multiplicity in 186 < PT < 254 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 multiplicity in 254 < PT < 326 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 multiplicity in 326 < PT < 408 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 multiplicity in 408 < PT < 481 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 multiplicity in 481 < PT < 614 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 multiplicity in 614 < PT < 800 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 multiplicity in 800 < PT < 1000 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 multiplicity in 1000 < PT < 4000 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 pTD2 in 50 < PT < 65 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 pTD2 in 65 < PT < 88 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 pTD2 in 88 < PT < 120 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 pTD2 in 120 < PT < 150 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 pTD2 in 150 < PT < 186 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 pTD2 in 186 < PT < 254 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 pTD2 in 254 < PT < 326 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 pTD2 in 326 < PT < 408 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 pTD2 in 408 < PT < 1500 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 pTD2 in 50 < PT < 65 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 pTD2 in 65 < PT < 88 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 pTD2 in 88 < PT < 120 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 pTD2 in 120 < PT < 150 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 pTD2 in 150 < PT < 186 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 pTD2 in 186 < PT < 254 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 pTD2 in 254 < PT < 326 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 pTD2 in 326 < PT < 408 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 pTD2 in 408 < PT < 1500 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 pTD2 in 50 < PT < 65 GeV in the central dijet region.
Particle-level distributions of groomed AK8 pTD2 in 65 < PT < 88 GeV in the central dijet region.
Particle-level distributions of groomed AK8 pTD2 in 88 < PT < 120 GeV in the central dijet region.
Particle-level distributions of groomed AK8 pTD2 in 120 < PT < 150 GeV in the central dijet region.
Particle-level distributions of groomed AK8 pTD2 in 150 < PT < 186 GeV in the central dijet region.
Particle-level distributions of groomed AK8 pTD2 in 186 < PT < 254 GeV in the central dijet region.
Particle-level distributions of groomed AK8 pTD2 in 254 < PT < 326 GeV in the central dijet region.
Particle-level distributions of groomed AK8 pTD2 in 326 < PT < 408 GeV in the central dijet region.
Particle-level distributions of groomed AK8 pTD2 in 408 < PT < 481 GeV in the central dijet region.
Particle-level distributions of groomed AK8 pTD2 in 481 < PT < 614 GeV in the central dijet region.
Particle-level distributions of groomed AK8 pTD2 in 614 < PT < 800 GeV in the central dijet region.
Particle-level distributions of groomed AK8 pTD2 in 800 < PT < 1000 GeV in the central dijet region.
Particle-level distributions of groomed AK8 pTD2 in 1000 < PT < 4000 GeV in the central dijet region.
Particle-level distributions of groomed AK8 pTD2 in 50 < PT < 65 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 pTD2 in 65 < PT < 88 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 pTD2 in 88 < PT < 120 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 pTD2 in 120 < PT < 150 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 pTD2 in 150 < PT < 186 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 pTD2 in 186 < PT < 254 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 pTD2 in 254 < PT < 326 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 pTD2 in 326 < PT < 408 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 pTD2 in 408 < PT < 481 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 pTD2 in 481 < PT < 614 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 pTD2 in 614 < PT < 800 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 pTD2 in 800 < PT < 1000 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 pTD2 in 1000 < PT < 4000 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 thrust in 50 < PT < 65 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 thrust in 65 < PT < 88 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 thrust in 88 < PT < 120 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 thrust in 120 < PT < 150 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 thrust in 150 < PT < 186 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 thrust in 186 < PT < 254 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 thrust in 254 < PT < 326 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 thrust in 326 < PT < 408 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 thrust in 408 < PT < 1500 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 thrust in 50 < PT < 65 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 thrust in 65 < PT < 88 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 thrust in 88 < PT < 120 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 thrust in 120 < PT < 150 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 thrust in 150 < PT < 186 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 thrust in 186 < PT < 254 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 thrust in 254 < PT < 326 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 thrust in 326 < PT < 408 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 thrust in 408 < PT < 1500 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 thrust in 50 < PT < 65 GeV in the central dijet region.
Particle-level distributions of groomed AK8 thrust in 65 < PT < 88 GeV in the central dijet region.
Particle-level distributions of groomed AK8 thrust in 88 < PT < 120 GeV in the central dijet region.
Particle-level distributions of groomed AK8 thrust in 120 < PT < 150 GeV in the central dijet region.
Particle-level distributions of groomed AK8 thrust in 150 < PT < 186 GeV in the central dijet region.
Particle-level distributions of groomed AK8 thrust in 186 < PT < 254 GeV in the central dijet region.
Particle-level distributions of groomed AK8 thrust in 254 < PT < 326 GeV in the central dijet region.
Particle-level distributions of groomed AK8 thrust in 326 < PT < 408 GeV in the central dijet region.
Particle-level distributions of groomed AK8 thrust in 408 < PT < 481 GeV in the central dijet region.
Particle-level distributions of groomed AK8 thrust in 481 < PT < 614 GeV in the central dijet region.
Particle-level distributions of groomed AK8 thrust in 614 < PT < 800 GeV in the central dijet region.
Particle-level distributions of groomed AK8 thrust in 800 < PT < 1000 GeV in the central dijet region.
Particle-level distributions of groomed AK8 thrust in 1000 < PT < 4000 GeV in the central dijet region.
Particle-level distributions of groomed AK8 thrust in 50 < PT < 65 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 thrust in 65 < PT < 88 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 thrust in 88 < PT < 120 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 thrust in 120 < PT < 150 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 thrust in 150 < PT < 186 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 thrust in 186 < PT < 254 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 thrust in 254 < PT < 326 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 thrust in 326 < PT < 408 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 thrust in 408 < PT < 481 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 thrust in 481 < PT < 614 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 thrust in 614 < PT < 800 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 thrust in 800 < PT < 1000 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 thrust in 1000 < PT < 4000 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 width in 50 < PT < 65 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 width in 65 < PT < 88 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 width in 88 < PT < 120 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 width in 120 < PT < 150 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 width in 150 < PT < 186 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 width in 186 < PT < 254 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 width in 254 < PT < 326 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 width in 326 < PT < 408 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 width in 408 < PT < 1500 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 width in 50 < PT < 65 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 width in 65 < PT < 88 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 width in 88 < PT < 120 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 width in 120 < PT < 150 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 width in 150 < PT < 186 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 width in 186 < PT < 254 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 width in 254 < PT < 326 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 width in 326 < PT < 408 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK8 width in 408 < PT < 1500 GeV in the Z+jet region.
Particle-level distributions of groomed AK8 width in 50 < PT < 65 GeV in the central dijet region.
Particle-level distributions of groomed AK8 width in 65 < PT < 88 GeV in the central dijet region.
Particle-level distributions of groomed AK8 width in 88 < PT < 120 GeV in the central dijet region.
Particle-level distributions of groomed AK8 width in 120 < PT < 150 GeV in the central dijet region.
Particle-level distributions of groomed AK8 width in 150 < PT < 186 GeV in the central dijet region.
Particle-level distributions of groomed AK8 width in 186 < PT < 254 GeV in the central dijet region.
Particle-level distributions of groomed AK8 width in 254 < PT < 326 GeV in the central dijet region.
Particle-level distributions of groomed AK8 width in 326 < PT < 408 GeV in the central dijet region.
Particle-level distributions of groomed AK8 width in 408 < PT < 481 GeV in the central dijet region.
Particle-level distributions of groomed AK8 width in 481 < PT < 614 GeV in the central dijet region.
Particle-level distributions of groomed AK8 width in 614 < PT < 800 GeV in the central dijet region.
Particle-level distributions of groomed AK8 width in 800 < PT < 1000 GeV in the central dijet region.
Particle-level distributions of groomed AK8 width in 1000 < PT < 4000 GeV in the central dijet region.
Particle-level distributions of groomed AK8 width in 50 < PT < 65 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 width in 65 < PT < 88 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 width in 88 < PT < 120 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 width in 120 < PT < 150 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 width in 150 < PT < 186 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 width in 186 < PT < 254 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 width in 254 < PT < 326 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 width in 326 < PT < 408 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 width in 408 < PT < 481 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 width in 481 < PT < 614 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 width in 614 < PT < 800 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 width in 800 < PT < 1000 GeV in the forward dijet region.
Particle-level distributions of groomed AK8 width in 1000 < PT < 4000 GeV in the forward dijet region.
The polarization transfer κ 0 and the tensor analyzing power T 20 for the 1 H d p)d reaction have been measured up to an internal momentum of k = 0.58 GeV/c. Comparison of the same observables obtained in recent studies for 1 H d p)d reaction, as a function of k , show different behavior. However the data from these two reactions are almost identical when compared in T 20 versus κ 0 correlation plots. We discuss similarities and differences observed in the two reactions.
The authors use the Infinite Momentum Frame variable K= M( proton) * sqrt(1/(4*a*(1-a)) - 1), where a = (E(proton)+P_long(proton))/(E(deut)+P(deut)).
We present first data on sub-threshold production of K0 s mesons and {\Lambda} hyperons in Au+Au collisions at $\sqrt{s_{NN}}$ = 2.4 GeV. We observe an universal <Apart> scaling of hadrons containing strangeness, independent of their corresponding production thresholds. Comparing the yields, their <Apart> scaling, and the shapes of the rapidity and the pt spectra to state-of-the-art transport model (UrQMD, HSD, IQMD) predictions, we find that none of the latter can simultaneously describe all observables with reasonable \c{hi}2 values.
Example of $K^{0}_{S}$ signal for 0-40% most central events, over mixed-event background for the bin $-0.05 < y_{cm} < 0.05$ and reduced transverse masses between $80-120 MeV/c^{2}$.
Example of $K^{0}_{S}$ signal for 0-40% most central events, over mixed-event background for the bin $-0.05 < y_{cm} < 0.05$ and reduced transverse masses between $80-120 MeV/c^{2}$.
Example of $\Lambda$ signal for 0-40% most central events, over mixed-event background for the bin $-0.05 < y_{cm} < 0.05$ and reduced transverse masses between $100-150 MeV/c^{2}$.
Example of $\Lambda$ signal for 0-40% most central events, over mixed-event background for the bin $-0.05 < y_{cm} < 0.05$ and reduced transverse masses between $100-150 MeV/c^{2}$.
Reduced transverse mass ($m_{t}-m_{0}$) spectra of $K^{0}_{S}$ for the 0-40% most central events.
Reduced transverse mass ($m_{t}-m_{0}$) spectra of $K^{0}_{S}$ for the 0-40% most central events. NOTE: The spectra are not scaled by $1/N_{Events}$! To compare the data, divide by $N_{Events} = 2.1997626 x 10^{9}$
Reduced transverse mass ($m_{t}-m_{0}$) spectra of $\Lambda$ for the 0-40% most central events.
Reduced transverse mass ($m_{t}-m_{0}$) spectra of $\Lambda$ for the 0-40% most central events. NOTE: The spectra are not scaled by $1/N_{Events}$! To compare the data, divide by $N_{Events} = 2.1997626 x 10^{9}$
Rapidity distribution of $K^{0}_{S}$
Rapidity distribution of $K^{0}_{S}$
Rapidity distribution of $\Lambda$
Rapidity distribution of $\Lambda$
Compilation of mid-rapidity yields for central Au+Au collisions as a function of $\sqrt{s_{NN}}$ of $K^{0}_{S}$ and $\Lambda$.
Compilation of mid-rapidity yields for central Au+Au collisions as a function of $\sqrt{s_{NN}}$ of $K^{0}_{S}$ and $\Lambda$.
Multiplicities per mean number of participants $Mult/\langle A_{Part}\rangle$ as a function of $\langle A_{Part}\rangle$
Multiplicities per mean number of participants $Mult/\langle A_{Part}\rangle$ as a function of $\langle A_{Part}\rangle$
Multiplicities per mean number of participants $Mult/\langle A_{Part}\rangle$ as a function of $\langle A_{Part}\rangle$ for $K^{0}_{S}$
Multiplicities per mean number of participants $Mult/\langle A_{Part}\rangle$ as a function of $\langle A_{Part}\rangle$ for $K^{0}_{S}$
Multiplicities per mean number of participants $Mult/\langle A_{Part}\rangle$ as a function of $\langle A_{Part}\rangle$ for $\Lambda$
Multiplicities per mean number of participants $Mult/\langle A_{Part}\rangle$ as a function of $\langle A_{Part}\rangle$ for $\Lambda$
Comparison of the shape of the rapidity distribution of $K^{0}_{S}$ to various transport model versions.
Comparison of the shape of the rapidity distribution of $K^{0}_{S}$ to various transport model versions.
Comparison of the shape of the rapidity distribution of $\Lambda$ to various transport model versions.
Comparison of the shape of the rapidity distribution of $\Lambda$ to various transport model versions.
Comparison of the shape of the $p_{t}$-spectra for $\pm0.15$ rapidity units around mid-rapidity of $K^{0}_{S}$ to various transport model versions.
Comparison of the shape of the $p_{t}$-spectra for $\pm0.15$ rapidity units around mid-rapidity of $K^{0}_{S}$ to various transport model versions.
Comparison of the shape of the $p_{t}$-spectra for $\pm0.15$ rapidity units around mid-rapidity of $\Lambda$ to various transport model versions.
Comparison of the shape of the $p_{t}$-spectra for $\pm0.15$ rapidity units around mid-rapidity of $\Lambda$ to various transport model versions.
Differential yield of $K^{0}_{S}$ as function of rapdidity and reduced transverse mass for the four centrality classes.
Differential yield of $K^{0}_{S}$ as function of rapdidity and reduced transverse mass for the four centrality classes. NOTE: The spectra are not scaled by $1/N_{Events}$! To compare the data, divide by $N_{Events} = 5.64247975 x 10^{8} (0 - 10\%)$, $5.85743394 x 10^{8} (10 - 20\%)$, $5.76369451 x 10^{8} (20 - 30\%)$ or $4.73401752 x 10^{8} (30 - 40\%)$
Differential yield of $\Lambda$ as function of rapdidity and reduced transverse mass for the four centrality classes.
Differential yield of $\Lambda$ as function of rapdidity and reduced transverse mass for the four centrality classes. NOTE: The spectra are not scaled by $1/N_{Events}$! To compare the data, divide by $N_{Events} = 5.64247975 x 10^{8} (0 - 10\%)$, $5.85743394 x 10^{8} (10 - 20\%)$, $5.76369451 x 10^{8} (20 - 30\%)$ or $4.73401752 x 10^{8} (30 - 40\%)$
A measurement of observables sensitive to effects of colour reconnection in top-quark pair-production events is presented using 139 fb$^{-1}$ of 13$\,$TeV proton-proton collision data collected by the ATLAS detector at the LHC. Events are selected by requiring exactly one isolated electron and one isolated muon with opposite charge and two or three jets, where exactly two jets are required to be $b$-tagged. For the selected events, measurements are presented for the charged-particle multiplicity, the scalar sum of the transverse momenta of the charged particles, and the same scalar sum in bins of charged-particle multiplicity. These observables are unfolded to the stable-particle level, thereby correcting for migration effects due to finite detector resolution, acceptance and efficiency effects. The particle-level measurements are compared with different colour reconnection models in Monte Carlo generators. These measurements disfavour some of the colour reconnection models and provide inputs to future optimisation of the parameters in Monte Carlo generators.
Naming convention for the observables at different levels of the analysis. At the background-subtracted level the contributions of tracks from pile-up collisions and tracks from secondary vertices are subtracted. At the corrected level the tracking-efficiency correction (TEC) is applied. The observables at particle level are the analysis results.
The $\chi^2$ and NDF for measured normalised differential cross-sections obtained by comparing the different predictions with the unfolded data. Global($n_\text{ch},\Sigma_{n_{\text{ch}}} p_{\text{T}}$) denotes the scenario in which the covariance matrix is built including the correlations of systematic uncertainties between the two observables $n_{\text{ch}}$ and $\Sigma_{n_{\text{ch}}} p_{\text{T}}$
Normalised differential cross-section as a function of $n_\text{ch}$.
Normalised differential cross-section as a function of $\sum_{n_{\text{ch}}} p_{\text{T}}$.
Normalised double-differential cross-section as a function of $\sum_{n_{\text{ch}}} p_{\text{T}}$ vs. $n_\text{ch}$ in $n_\text{ch} < 20$.
Normalised double-differential cross-section as a function of $\sum_{n_{\text{ch}}} p_{\text{T}}$ vs. $n_\text{ch}$ in $ 20 \leq n_\text{ch} < 40$.
Normalised double-differential cross-section as a function of $\sum_{n_{\text{ch}}} p_{\text{T}}$ vs. $n_\text{ch}$ in $ 40 \leq n_\text{ch} < 60$.
Normalised double-differential cross-section as a function of $\sum_{n_{\text{ch}}} p_{\text{T}}$ vs. $n_\text{ch}$ in $ 60 \leq n_\text{ch} < 80$.
Normalised double-differential cross-section as a function of $\sum_{n_{\text{ch}}} p_{\text{T}}$ vs. $n\text{ch}$ in $ n_\text{ch} \geq 80$.
The $\chi^2$ and NDF for measured absolute differential cross-sections obtained by comparing the different predictions with the unfolded data. Global($n_\text{ch},\Sigma_{n_{\text{ch}}} p_{\text{T}}$) denotes the scenario in which the covariance matrix is built including the correlations of systematic uncertainties between the two observables $n_{\text{ch}}$ and $\Sigma_{n_{\text{ch}}} p_{\text{T}}$
Absolute differential cross-section as a function of $n_\text{ch}$.
Absolute differential cross-section as a function of $\sum_{n_{\text{ch}}} p_{\text{T}}$.
Absolute double-differential cross-section as a function of $\sum_{n_{\text{ch}}} p_{\text{T}}$ vs. $n_\text{ch}$ in $n_\text{ch} < 20$.
Absolute double-differential cross-section as a function of $\sum_{n_{\text{ch}}} p_{\text{T}}$ vs. $n_\text{ch}$ in $ 20 \leq n_\text{ch} < 40$.
Absolute double-differential cross-section as a function of $\sum_{n_{\text{ch}}} p_{\text{T}}$ vs. $n_\text{ch}$ in $ 40 \leq n_\text{ch} < 60$.
Absolute double-differential cross-section as a function of $\sum_{n_{\text{ch}}} p_{\text{T}}$ vs. $n_\text{ch}$ in $ 60 \leq n_\text{ch} < 80$.
Absolute double-differential cross-section as a function of $\sum_{n_{\text{ch}}} p_{\text{T}}$ vs. $n\text{ch}$ in $ n_\text{ch} \geq 80$.
The results from the first kinematically complete measurement of the dd --> 4Hepipi reaction are reported. The aim was to investigate a long standing puzzle regarding the origin of the peculiar pipi-invariant mass distributions appearing in double pion production in light ion collisions, the so-called ABC effect. The measurements were performed at the incident deuteron energies of 712 MeV and 1029 MeV, with the WASA detector assembly at CELSIUS in Uppsala, Sweden. We report the observation of a characteristic enhancement at low pipi-invariant mass at 712 MeV, the lowest energy yet. At the higher energy, in addition to confirming previous experimental observations, our results reveal a strong angular dependence of the pions in the overall centre of mass system. The results are qualitatively reproduced by a theoretical model, according to which the ABC effect is described as resulting from a kinematical enhancement in the production of the pion pairs from two parallel and independent NN--> dpi sub-processes.
Total cross section for neutral and charged pion channels.
Invariant PI0 PI0 mass distribution at deuteron kinetic energy 1.029 GeV.
Invariant PI+ PI- mass distribution at deuteron kinetic energy 1.029 GeV.
Invariant HE4 PI0 mass distribution at deuteron kinetic energy 1.029 GeV.
Invariant HE4 PI+ mass distribution at deuteron kinetic energy 1.029 GeV.
Invariant HE4 PI- mass distribution at deuteron kinetic energy 1.029 GeV.
Angular distributions of HE4 at incident deuteron energy of 1.029 GeV in the neutral pion channel.
Angular distributions of PI0 at incident deuteron energy of 1.029 GeV in the neutral pion channel.
Angular distributions of PI0 at incident deuteron energy of 1.029 GeV in the neutral pion channel.
Angular distributions of PI0 at incident deuteron energy of 1.029 GeV in the neutral pion channel.
Angular distributions of HE4 at incident deuteron energy of 1.029 GeV in the charged pion channel.
Angular distributions of PI+ at incident deuteron energy of 1.029 GeV in the charged pion channel.
Angular distributions of PI- at incident deuteron energy of 1.029 GeV in the charged pion channel.
Angular distributions of PI+ PI- at incident deuteron energy of 1.029 GeV in the charged pion channel.
Angular distributions of PI+ PI- at incident deuteron energy of 1.029 GeV in the charged pion channel.
The first spin-transfer observables for the πd→pp reaction have been measured at a number of energies spanning the Δ resonance in this system. These parameters correspond to KSL and KSS of the pp→dπ reaction for incident proton energies ranging from 600 to 800 MeV. Such data can provide an important constraint on the determination of the partial-wave amplitudes describing this fundamental reaction. The discrepancies between our data, theoretical predictions, and values calculated from published partial-wave amplitudes demonstrate the need for further work in this area.
No description provided.
No description provided.
The polarization observable I^s, a feature exclusive to the acoplanar kinematics of multi-meson final states produced via linearly polarized photons, has been measured for the first time. Results for the reaction g p -> p pi0 eta are presented for incoming photon energies between 970 MeV and 1650 MeV along with the beam asymmetry I^c. The comparably large asymmetries demonstrate a high sensitivity of I^s to the dynamics of the reaction. Fits using Bonn-Gatchina partial wave analysis demonstrate that the new polarization observables carry significant information on the contributing partial waves.
Measured beam asymmetry I_S as a function of the angle between the reaction plane and the plane of the two final state particles with the the proton as the recoiling particle for the cm energy range 1642 to 1770 MeV.
Measured beam asymmetry I_S as a function of the angle between the reaction plane and the plane of the two final state particles with the the proton as the recoiling particle for the cm energy range 1770 to 1898 MeV.
Measured beam asymmetry I_S as a function of the angle between the reaction plane and the plane of the two final state particles with the the proton as the recoiling particle for the cm energy range 1898 to 1994 MeV.
Measured beam asymmetry I_S as a function of the angle between the reaction plane and the plane of the two final state particles with the the pi0 as the recoiling particle for the cm energy range 1642 to 1770 MeV.
Measured beam asymmetry I_S as a function of the angle between the reaction plane and the plane of the two final state particles with the the pi0 as the recoiling particle for the cm energy range 1770 to 1898 MeV.
Measured beam asymmetry I_S as a function of the angle between the reaction plane and the plane of the two final state particles with the the pi0 as the recoiling particle for the cm energy range 1898 to 1994 MeV.
Measured beam asymmetry I_S as a function of the angle between the reaction plane and the plane of the two final state particles with the the eta as the recoiling particle for the cm energy range 1642 to 1770 MeV.
Measured beam asymmetry I_S as a function of the angle between the reaction plane and the plane of the two final state particles with the the eta as the recoiling particle for the cm energy range 1770 to 1898 MeV.
Measured beam asymmetry I_S as a function of the angle between the reaction plane and the plane of the two final state particles with the the eta as the recoiling particle for the cm energy range 1898 to 1994 MeV.
Measured beam asymmetry I_C as a function of the angle between the reaction plane and the plane of the two final state particles with the the proton as the recoiling particle for the cm energy range 1642 to 1770 MeV.
Measured beam asymmetry I_C as a function of the angle between the reaction plane and the plane of the two final state particles with the the proton as the recoiling particle for the cm energy range 1770 to 1898 MeV.
Measured beam asymmetry I_C as a function of the angle between the reaction plane and the plane of the two final state particles with the the proton as the recoiling particle for the cm energy range 1898 to 1994 MeV.
Measured beam asymmetry I_C as a function of the angle between the reaction plane and the plane of the two final state particles with the the pi0 as the recoiling particle for the cm energy range 1642 to 1770 MeV.
Measured beam asymmetry I_C as a function of the angle between the reaction plane and the plane of the two final state particles with the the pi0 as the recoiling particle for the cm energy range 1770 to 1898 MeV.
Measured beam asymmetry I_C as a function of the angle between the reaction plane and the plane of the two final state particles with the the pi0 as the recoiling particle for the cm energy range 1898 to 1994 MeV.
Measured beam asymmetry I_C as a function of the angle between the reaction plane and the plane of the two final state particles with the the eta as the recoiling particle for the cm energy range 1642 to 1770 MeV.
Measured beam asymmetry I_C as a function of the angle between the reaction plane and the plane of the two final state particles with the the eta as the recoiling particle for the cm energy range 1770 to 1898 MeV.
Measured beam asymmetry I_C as a function of the angle between the reaction plane and the plane of the two final state particles with the the eta as the recoiling particle for the cm energy range 1898 to 1994 MeV.
In photoproduction experiments, a large number of final states yielding various resonance contributions are accessible. To extract resonance parameters via partial-wave analysis not only the measurement of differential cross-sections is necessary, but also the determination of polarization observables. At the electron accelerator ELSA (Bonn) the coherent bremsstrahlung method was used to generate a linearly polarized photon beam. Using the CBELSA/TAPS detector setup, the beam asymmetry Σ in the reaction γp → pπ 0 η was determined as a function of various masses and angles for photon energies between 970MeV and 1650MeV.
Measured beam asymmetry as a function of the cosine of the scattered proton angle for beam energies 0.970 to 1.200 GeV.
Measured beam asymmetry as a function of the cosine of the scattered proton angle for beam energies 1.200 to 1.450 GeV.
Measured beam asymmetry as a function of the cosine of the scattered proton angle for beam energies 1.450 to 1.650 GeV.
Measured beam asymmetry as a function of the invariant mass of the PI0-ETA system for beam energies 0.970 to 1.200 GeV.
Measured beam asymmetry as a function of the invariant mass of the PI0-ETA system for beam energies 1.200 to 1.450 GeV.
Measured beam asymmetry as a function of the invariant mass of the PI0-ETA system for beam energies 1.450 to 1.650 GeV.
Measured beam asymmetry as a function of the invariant mass of the P-PI0 system for beam energies 0.970 to 1.200 GeV.
Measured beam asymmetry as a function of the invariant mass of the P-PI0 system for beam energies 1.200 to 1.450 GeV.
Measured beam asymmetry as a function of the invariant mass of the P-PI0 system for beam energies 1.450 to 1.650 GeV.
Measured beam asymmetry as a function of the invariant mass of the P-ETA system for beam energies 0.970 to 1.200 GeV.
Measured beam asymmetry as a function of the invariant mass of the P-ETA system for beam energies 1.200 to 1.450 GeV.
Measured beam asymmetry as a function of the invariant mass of the P-ETA system for beam energies 1.450 to 1.650 GeV.
The spin-dependent observables N 0 s ″ kn , D 0 n 0 n and K 0 s ″ k 0 in pp elastic scattering were measured at nine energies between 0.84 and 2.1 GeV using the SATURNE II polarized proton beam and the Saclay frozen spin polarized target. The beam polarization was oriented longitudinally and the target polarization was oriented vertically. Precession of the recoil particle spin in the target holding field introduces a small contribution from other parameters. The present results for K 0 s ″ k 0 and D 0 n 0 n agree with our previous measurements of the same observables carried out in different beam and target spin configurations as well as with previously existing measurements. The observable N 0 s ″ kn had not been measured previously above 0.58 GeV. Below 1.3 GeV our data are compared with the predictions of the Saclay-Geneva phase shift analysis. The new results will considerably affect the phase shift analysis solutions and will contribute to their extension towards higher energies.
No description provided.
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Tensor polarization observables (t20, t21 and t22) have been measured in elastic electron-deuteron scattering for six values of momentum transfer between 0.66 and 1.7 (GeV/c)^2. The experiment was performed at the Jefferson Laboratory in Hall C using the electron HMS Spectrometer, a specially designed deuteron magnetic channel and the recoil deuteron polarimeter POLDER. The new data determine to much larger Q^2 the deuteron charge form factors G_C and G_Q. They are in good agreement with relativistic calculations and disagree with pQCD predictions.
No description provided.
No description provided.
No description provided.
Statistical and systematic errors are combined on quadratures.
Statistical and systematic errors are combined on quadratures.
In this Report, QCD results obtained from a study of hadronic event structure in high energy e^+e^- interactions with the L3 detector are presented. The operation of the LEP collider at many different collision energies from 91 GeV to 209 GeV offers a unique opportunity to test QCD by measuring the energy dependence of different observables. The main results concern the measurement of the strong coupling constant, \alpha_s, from hadronic event shapes and the study of effects of soft gluon coherence through charged particle multiplicity and momentum distributions.
Jet fractions using the JADE algorithm as a function of the jet resolution parameter YCUT at c.m. energy 130.1 GeV.
Jet fractions using the JADE algorithm as a function of the jet resolution parameter YCUT at c.m. energy 136.1 GeV.
Jet fractions using the JADE algorithm as a function of the jet resolution parameter YCUT at c.m. energy 161.3 GeV.
Jet fractions using the JADE algorithm as a function of the jet resolution parameter YCUT at c.m. energy 172.3 GeV.
Jet fractions using the JADE algorithm as a function of the jet resolution parameter YCUT at c.m. energy 182.8 GeV.
Jet fractions using the JADE algorithm as a function of the jet resolution parameter YCUT at c.m. energy 188.6 GeV.
Jet fractions using the JADE algorithm as a function of the jet resolution parameter YCUT at c.m. energy 194.4 GeV.
Jet fractions using the JADE algorithm as a function of the jet resolution parameter YCUT at c.m. energy 200.2 GeV.
Jet fractions using the JADE algorithm as a function of the jet resolution parameter YCUT at c.m. energy 206.2 GeV.
Jet fractions using the KT(Durham) algorithm as a function of the jet resolution parameter YCUT at c.m. energy 130.1 GeV.
Jet fractions using the KT(Durham) algorithm as a function of the jet resolution parameter YCUT at c.m. energy 136.1 GeV.
Jet fractions using the KT(Durham) algorithm as a function of the jet resolution parameter YCUT at c.m. energy 161.3 GeV.
Jet fractions using the KT(Durham) algorithm as a function of the jet resolution parameter YCUT at c.m. energy 172.3 GeV.
Jet fractions using the KT(Durham) algorithm as a function of the jet resolution parameter YCUT at c.m. energy 182.8 GeV.
Jet fractions using the KT(Durham) algorithm as a function of the jet resolution parameter YCUT at c.m. energy 188.6 GeV.
Jet fractions using the KT(Durham) algorithm as a function of the jet resolution parameter YCUT at c.m. energy 194.4 GeV.
Jet fractions using the KT(Durham) algorithm as a function of the jet resolution parameter YCUT at c.m. energy 200.2 GeV.
Jet fractions using the KT(Durham) algorithm as a function of the jet resolution parameter YCUT at c.m. energy 206.2 GeV.
Jet fractions using the Cambridge algorithm as a function of the jet resolution parameter YCUT at c.m. energy 202.2 GeV.
Jet fractions using the Cambridge algorithm as a function of the jet resolution parameter YCUT at c.m. energy 206.2 GeV.
Differential distributions for event thrust.
Differential distributions for event thrust.
Differential distributions for event thrust.
Differential distributions for event thrust.
Differential distributions for event thrust.
Differential distributions for the scaled heavy jet mass (RHO(C=HEAVY)).
Differential distributions for the scaled heavy jet mass (RHO(C=HEAVY)).
Differential distributions for the scaled heavy jet mass (RHO(C=HEAVY)).
Differential distributions for the scaled heavy jet mass (RHO(C=HEAVY)).
Differential distributions for the scaled heavy jet mass (RHO(C=HEAVY)).
Differential distributions for total jet broadening (BT).
Differential distributions for total jet broadening (BT).
Differential distributions for total jet broadening (BT).
Differential distributions for total jet broadening (BT).
Differential distributions for total jet broadening (BT).
Differential distributions for wide jet broadening (BW).
Differential distributions for wide jet broadening (BW).
Differential distributions for wide jet broadening (BW).
Differential distributions for wide jet broadening (BW).
Differential distributions for wide jet broadening (BW).
Differential distributions for the C-Parameter.
Differential distributions for the C-Parameter.
Differential distributions for the C-Parameter.
Differential distributions for the D-Parameter.
Differential distributions for the D-Parameter.
Differential distributions for the D-Parameter.
Differential distributions for the THRUST at c.m. energy 91.2 GeV for light quark (udsc) and b quark events.
Differential distributions for the RHO(C=HEAVY) at c.m. energy 91.2 GeV forlight quark (udsc) and b quark events.
Differential distributions for the BT at c.m. energy 91.2 GeV for light quark (udsc) and b quark events.
Differential distributions for the BW at c.m. energy 91.2 GeV for light quark (udsc) and b quark events.
Differential distributions for the C-PARAM at c.m. energy 91.2 GeV for light quark (udsc) and b quark events.
Differential distributions for the D-PARAM at c.m. energy 91.2 GeV for light quark (udsc) and b quark events.
Mean values (first moment) and dispersion (second moment) of the THRUST distribution as a function of c.m. energy.
Mean values (first moment) and dispersion (second moment) of the scaled heavy jet mass (RHO(C=HEAVY)) as a function of c.m. energy.
Mean values (first moment) and dispersion (second moment) of the total jet broadening (BT) as a function of c.m. energy.
Mean values (first moment) and dispersion (second moment) of the wide jet broadening (BW) as a function of c.m. energy.
Mean values (first moment) and dispersion (second moment) of the C-PARAM as a function of c.m. energy.
Mean values (first moment) and dispersion (second moment) of the D-PARAM as a function of c.m. energy.
Charged particle multiplicities at c.m. energy 91.2 GeV for all flavour, light quark (udsc) and bottom (b) flavour events.
Charged particle multiplicity.
Charged particle multiplicity.
Charged particle multiplicity.
First and second moment of the charged particle multiplicity distribution at c.m. energy 91.2 GeV for all flavours and for udsc an b flavours.
First and second moment of the charged particle multiplicity distribution at c.m. energy.
Distribution of LN(1/X) at c.m. energy 91.2 GeV.
Distribution of LN(1/X) at higher c.m. energies.
Distribution of LN(1/X) at higher c.m. energies.
Distribution of LN(1/X) at higher c.m. energies.
The differential cross section and deuteron analysing powers of the dp -> {pp}n charge-exchange reaction have been measured with the ANKE spectrometer at the COSY storage ring. Using a deuteron beam of energy 1170 MeV, data were obtained for small momentum transfers to a {pp} system with low excitation energy. A good quantitative understanding of all the measured observables is provided by the impulse approximation using known neutron-proton amplitudes. The proof of principle achieved here for the method suggests that measurements at higher energies will provide useful information in regions where the existing np database is far less reliable.
Differential cross section for the unpolarized DEUT P --> P P N reaction integrated over momentum transfer Q < 100 MeV.
Unpolarized differential cross section for the DEUT P --> P P N reaction of (P P) excitation energies < 3 MeV.
Spherical tensor analysing powers t20 and t22 for EPP 0.1 to 1.0 MeV and cos(theta) > 0.5.
Spherical tensor analysing powers t20 and t22 for EPP 0.1 to 1.0 MeV and cos(theta) < 0.5.
Spherical tensor analysing powers t20 and t22 for EPP 1 to 3 MeV and cos(theta) > 0.5.
Spherical tensor analysing powers t20 and t22 for EPP 1 to 3 MeV and cos(theta) < 0.5.
An updated analysis using about 1.5 million events recorded at $\sqrt{s} = M_Z$ with the DELPHI detector in 1994 is presented. Eighteen infrared and collinear safe event shape observables are measured as a function of the polar angle of the thrust axis. The data are compared to theoretical calculations in ${\cal O} (\alpha_s^2)$ including the event orientation. A combined fit of $\alpha_s$ and of the renormalization scale $x_{\mu}$ in $\cal O(\alpha_s^2$) yields an excellent description of the high statistics data. The weighted average from 18 observables including quark mass effects and correlations is $\alpha_s(M_Z^2) = 0.1174 \pm 0.0026$. The final result, derived from the jet cone energy fraction, the observable with the smallest theoretical and experimental uncertainty, is $\alpha_s(M_Z^2) = 0.1180 \pm 0.0006 (exp.) \pm 0.0013 (hadr.) \pm 0.0008 (scale) \pm 0.0007 (mass)$. Further studies include an $\alpha_s$ determination using theoretical predictions in the next-to-leading log approximation (NLLA), matched NLLA and $\cal O(\alpha_s^2$) predictions as well as theoretically motivated optimized scale setting methods. The influence of higher order contributions was also investigated by using the method of Pad\'{e} approximants. Average $\alpha_s$ values derived from the different approaches are in good agreement.
The weighted value of ALPHA-S from all the measured observables using experimentally optimized renormalization scale values and corrected for the b-mass toleading order.
The value of ALPHA-S derived from the JCEF and corrected for heavy quark mass effects. The quoted errors are respectively due to experimental error, hadronization, renormalization scale and heavy quark mass correction uncertainties.
Energy Energy Correlation EEC.
Asymmetry of the Energy Energy Correlation AEEC.
Jet Cone Energy Fraction.
1 - Thrust (1-T).
Oblateness O.
C-Parameter C.
Heavy Jet Mass.
Sum of the Jet Masses.
Difference of the Jet Masses.
Wide Jet Broadening BMAX.
Total Jet Broadening BSUM.
Differential 2-Jet Rate E0 Scheme D2(E0).
Differential 2-Jet Rate P0 Scheme D2(P0).
Differential 2-Jet Rate P Scheme D2(P).
Differential 2-Jet Rate Jade Alogrithm D2(Jad).
Differential 2-Jet Rate Durham Alogrithm D2(Dur).
Differential 2-Jet Rate Geneva Alogrithm D2(Gen).
Differential 2-Jet Rate Cambridge Alogrithm D2(Cam).
Energy Energy Correlation EEC.
Energy Energy Correlation EEC.
Energy Energy Correlation EEC.
Energy Energy Correlation EEC.
Asymmetry of the Energy Energy Correlation AEEC.
Asymmetry of the Energy Energy Correlation AEEC.
Asymmetry of the Energy Energy Correlation AEEC.
Asymmetry of the Energy Energy Correlation AEEC.
Jet Cone Energy Fraction.
Jet Cone Energy Fraction.
Jet Cone Energy Fraction.
Jet Cone Energy Fraction.
1 - Thrust (1-T).
The angular distributions of the cross section, the proton analyzing power, and all proton polarization transfer coefficients of p→d elastic scattering were measured at 250 MeV. The range of center-of-mass angles was 10°–165° for the cross section and the analyzing power, and about 10°–95° for the polarization transfer coefficients. These are the first measurements of a complete set of proton polarization observables for p→d elastic scattering at intermediate energies. The present data are compared with theoretical predictions based on exact solutions of the three-nucleon Faddeev equations and modern realistic nucleon-nucleon potentials combined with three-nucleon forces (3NF), namely, the Tucson-Melbourne (TM) 2π-exchange model, a modification thereof (TM′) closer to chiral symmetry, and the Urbana IX model. Large effects of the three-nucleon forces are predicted. The inclusion of the three-nucleon forces gives a good description of the cross section at angles below the minimum. However, appreciable discrepancies between the data and predictions remain at backward angles. For the spin observables the predictions of the TM 3NF model deviate strongly from the other two 3NF models, which are close together, except for Kyy′. In the case of the analyzing power all 3NF models fail to describe the data at the upper half of the angular range. In the restricted measured angular range the polarization transfer coefficients are fairly well described by the TM′ and Urbana IX 3NF models, whereas the TM 3NF model mostly fails. The transfer coefficient Kyy′ is best described by the Urbana IX but the theoretical description is still insufficient to reproduce the experimental data. These results call for a better understanding of the spin structure of the three-nucleon force and very likely for a full relativistic treatment of the three-nucleon continuum.
Cross section and analyzing power measurements.
Proton polarization transfer coefficients.
The spin correlation parameters A 00 kk and A 00 sk were measured at 0.874, 0.934, 1.095, 1.295, 1.596, 1.796, 2.096, and 2.396 GeV, using the SATURNE II polarized proton beam and tha Saclay frozen spin polarized target. The present results for beam-target spin correlations obtained during measurements of three-spin index observables confirm, in particular, relatively large positive values of A 00 sk at certain energies and angles, as was shown in previously published data from a dedicated experiment.
No description provided.
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Results are presented for the spin-spin correlation parameters CSS and CLS for free np elastic scattering at neutron beam kinetic energies of 484, 634, 720, and 788 MeV and c.m. angles between 25° and 80°. The measurements were performed with a polarized neutron beam and a polarized proton target. These are the first measurements of this type to be reported in the forward angular region with a free polarized neutron beam. The observables CSS and CLS are both small at all energies, except for CLS at 788 MeV, which is larger than phase-shift analysis predictions by more than one standard deviation for most of the measured points.
No description provided.
No description provided.
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Using the ARGUS detector at the e+e- storage ring DORIS II, we have searched for the real and imaginary part of the electric dipole formfactor d_tau of the tau lepton in the production of tau pairs at q^2=100 GeV^2. This is the first direct measurement of this CP violating formfactor. We applied the method of optimised observables which takes into account all available information on the observed tau decay products. No evidence for CP violation was found, and we derive the following results: Re(d_tau)=(1.6+-.9)*10^(-16) ecm and Im(d_tau)=(-0.2+-0.8)*10^(-16) ecm, where statistical and systematic errors have been combined.
Electric dipole moment in E(electric charge)*CM units. Systematic and statistical errors are added in quadrature.
The spin-dependent observables D 0 n 0 n and K 0 nn 0 in pp elastic scattering were measured at 11 energies between 0.84 and 2.7 GeV using the SATURNE II polarized proton beam and the Saclay frozen-spin polarized target. The beam and target polarizations were oriented along the normal to the scattering plane. Below 1 GeV the present data agree with previously existing measurements. Below 1.3 GeV they are compared with the predictions of the Saclay-Geneva phase-shift analysis. The results will improve the phase-shift analysis solutions and will contribute to their extension towards higher energies.
No description provided.
No description provided.
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A polarized proton beam extracted from SATURNE II and the Saclay polarized proton target were used to determine the spin correlation parameter Aoosk and the rescattering observablesKos″ so; Dos″ok, Nos″sn, andNonsk at 1.80 and 2.10 GeV. The beam polarization was oriented perpendicular to the beam direction in the horizontal scattering plane and the target polarization was directed either along the vertical axis or longitudinally. Left-right and up-down asymmetries in the second scattering were measured. A check for the beam optimization with the beam and target polarizations oriented vertically provided other observables, of which results forDonon andKonno at 1.80, 1.85, 2.04, and 2.10 GeV are listed here. The new data at 2.10 GeV suggest a smooth energy dependence of spin triplet scattering amplitudes at fixed angles in the vicinity of this energy.
Spin correlation parameter CSL measured with the beam polarisation measuredalong the +-S direction and the target polarisation along the +-L axis. Additional 4.3 PCT systematic normalisation uncertainty.
Measurement of the rescattering parameter KSS with the beam polarisation inthe +- S direction. Additional 6.7 PCT systematic error.
Measurement of the rescattering parameter KSS with the beam polarisation inthe +- S direction. Additional 6.7 PCT systematic error.
Measurement of the rescattering parameter HSNS with the beam polarisation in the +- S direction and the target polarisation in the +- N direction. Additional 7.4 PCT systematic error.
Measurement of the rescattering parameter HSNS with the beam polarisation in the +- S direction and the target polarisation in the +- N direction. Additional 7.4 PCT systematic error.
Measurement of the rescattering parameter DLS with the beam polarisation inthe +- S direction and the target polarisation in the +- L direction. Additional 6.7 PCT systematic error.
Measurement of the rescattering parameter DLS with the beam polarisation inthe +- S direction and the target polarisation in the +- L direction. Additional 6.7 PCT systematic error.
Measurement of the rescattering parameter HSLN with the beam polarisation in the +- S direction and the target polarisation in the +- L or +- N directions. Additional 7.4 PCT systematic uncertainty.
Measurement of the rescattering parameter HSLN with the beam polarisation in the +- S direction and the target polarisation in the +- L or +- N directions. Additional 7.4 PCT systematic uncertainty.
Measurement of the rescattering parameters DNN and KNN for the beam and target polarisations in the +- N directions. Additional 6.7 PCT systematic error.
Measurement of the rescattering parameters DNN and KNN for the beam and target polarisations in the +- N directions. Additional 6.7 PCT systematic error.
Measurement of the rescattering parameters DNN and KNN for the beam and target polarisations in the +- N directions. Additional 6.7 PCT systematic error.
Measurement of the rescattering parameters DNN and KNN for the beam and target polarisations in the +- N directions. Additional 6.7 PCT systematic error.
Dijet cross sections as functions of several jet observables are measured in photoproduction using the H1 detector at HERA. The data sample comprises e^+p data with an integrated luminosity of 34.9 pb^(-1). Jets are selected using the inclusive k_T algorithm with a minimum transverse energy of 25 GeV for the leading jet. The phase space covers longitudinal proton momentum fraction x_p and photon longitudinal momentum fraction x_gamma in the ranges 0.05<x_p<0.6 and 0.1<x_gamma<1. The predictions of next-to-leading order perturbative QCD, including recent photon and proton parton densities, are found to be compatible with the data in a wide kinematical range.
Differential ep cross section for dijet production as a function of the invariant mass of the two jets.
Differential ep cross section for dijet production as a function of the average transverse energy the two jets.
Differential ep cross section for dijet production as a function of the maximum transverse energy the leading jet.
Differential ep cross section for dijet production as a function of the average pseudorapidity the two jets in two transverse energy regions and in the Y region 0.1 to 0.5.
Differential ep cross section for dijet production as a function of the average pseudorapidity the two jets in two transverse energy regions and in the Y region 0.5 to 0.9.
Differential ep cross section for dijet production as a function of the photon momentum fraction X(C=GAMMA) in two regions of proton fractional momentum XP.
Differential ep cross section for dijet production as a function of the proton momentum fraction XP in two regions of photon fractional momentum X(C=GAMMA).
Differential ep cross section for dijet production as a function of the photon momentum fraction X(C=GAMMA) in two regions maximum jet transverseenergy.
Differential ep cross section for dijet production as a function of COS(THETA*) in two regions of fractional photon momentum fraction X(C=GAMMA).
Differential ep cross section for dijet production as a function of COS(THETA*) for dijet masses > 65 GeV in two regions of fractional photon momentum fraction X(C=GAMMA).
We present a total of 273 independent data points of the analyzing powers A oono (nP) and A ooon (nP) in a large angular interval at four energies between 0.477 and 0.940 GeV. The SATURNE II polarized beam of free neutrons obtained from the break-up of polarized deuterons was scattered on the polarized Saclay frozen-spin proton target. Part of the data was obtained with a CH 2 target. A comparison of the two measured observables allows one to determine the polarization of the neutron beam. The present results provide an important contribution to any future theoretical or phenomenological analysis.
No description provided.
No description provided.
Data from 97.7 to 123.4 degrees are combined beam and target analyzing powers.
Data from 97.7 to 123.4 degrees are combined beam and target analyzing powers.
Data from 97.7 to 123.4 degrees are combined beam and target analyzing powers.
No description provided.
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