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In this letter, measurements of the shared momentum fraction ($z_{\rm{g}}$) and the groomed jet radius ($R_{\rm{g}}$), as defined in the SoftDrop algorihm, are reported in \pp collisions at $\sqrt{s} = 200$ GeV collected by the STAR experiment. These substructure observables are differentially measured for jets of varying resolution parameters from $R = 0.2 - 0.6$ in the transverse momentum range $15 < p_{\rm{T, jet}} < 60$ GeV$/c$. These studies show that, in the $p_{\rm{T, jet}}$ range accessible at $\sqrt{s} = 200$ GeV and with increasing jet resolution parameter and jet transverse momentum, the $z_{\rm{g}}$ distribution asymptotically converges to the DGLAP splitting kernel for a quark radiating a gluon. The groomed jet radius measurements reflect a momentum-dependent narrowing of the jet structure for jets of a given resolution parameter, i.e., the larger the $p_{\rm{T, jet}}$, the narrower the first splitting. For the first time, these fully corrected measurements are compared to Monte Carlo generators with leading order QCD matrix elements and leading log in the parton shower, and to state-of-the-art theoretical calculations at next-to-leading-log accuracy. We observe that PYTHIA 6 with parameters tuned to reproduce RHIC measurements is able to quantitatively describe data, whereas PYTHIA 8 and HERWIG 7, tuned to reproduce LHC data, are unable to provide a simultaneous description of both $z_{\rm{g}}$ and $R_{\rm{g}}$, resulting in opportunities for fine parameter tuning of these models for \pp collisions at RHIC energies. We also find that the theoretical calculations without non-perturbative corrections are able to qualitatively describe the trend in data for jets of large resolution parameters at high $p_{\rm{T, jet}}$, but fail at small jet resolution parameters and low jet transverse momenta.
A measurement of novel event shapes quantifying the isotropy of collider events is performed in 140 fb$^{-1}$ of proton-proton collisions with $\sqrt s=13$ TeV centre-of-mass energy recorded with the ATLAS detector at CERN's Large Hadron Collider. These event shapes are defined as the Wasserstein distance between collider events and isotropic reference geometries. This distance is evaluated by solving optimal transport problems, using the 'Energy-Mover's Distance'. Isotropic references with cylindrical and circular symmetries are studied, to probe the symmetries of interest at hadron colliders. The novel event-shape observables defined in this way are infrared- and collinear-safe, have improved dynamic range and have greater sensitivity to isotropic radiation patterns than other event shapes. The measured event-shape variables are corrected for detector effects, and presented in inclusive bins of jet multiplicity and the scalar sum of the two leading jets' transverse momenta. The measured distributions are provided as inputs to future Monte Carlo tuning campaigns and other studies probing fundamental properties of QCD and the production of hadronic final states up to the TeV-scale.
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 $n_{\mathrm{jets}}$
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 width in 120 < PT < 150 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 LHA in 120 < PT < 150 GeV 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 614 < PT < 800 GeV in the central dijet region.
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 50 < PT < 65 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 326 < PT < 408 GeV in the forward dijet 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 65 < PT < 88 GeV in the central dijet region.
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 408 < PT < 1500 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 multiplicity in 481 < PT < 614 GeV in the forward dijet 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 408 < PT < 1500 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 pTD2 in 326 < PT < 408 GeV in the forward dijet 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 1000 < PT < 4000 GeV in the central dijet 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 65 < PT < 88 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 width in 150 < PT < 186 GeV in the forward dijet 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.
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 120 < PT < 150 GeV in the central dijet region.
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 50 < PT < 65 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 326 < PT < 408 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.
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 120 < PT < 150 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 ungroomed AK8 LHA in 50 < PT < 65 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 50 < PT < 65 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 1000 < PT < 4000 GeV in the central 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 150 < PT < 186 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 614 < PT < 800 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 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 326 < PT < 408 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.
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 88 < PT < 120 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 50 < PT < 65 GeV in the forward dijet region.
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 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 408 < PT < 1500 GeV in the Z+jet 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 326 < PT < 408 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 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 254 < PT < 326 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 150 < PT < 186 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 254 < PT < 326 GeV in the Z+jet 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 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 65 < PT < 88 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 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 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 186 < PT < 254 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 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 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 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 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 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 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 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 (charged-only) in 65 < PT < 88 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.
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 120 < PT < 150 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.
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 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 65 < PT < 88 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 614 < PT < 800 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 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 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 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 120 < PT < 150 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 1000 < PT < 4000 GeV in the central 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 254 < PT < 326 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 pTD2 (charged-only) in 65 < PT < 88 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 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.
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 408 < PT < 481 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 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 408 < PT < 481 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 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 326 < PT < 408 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.
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 150 < PT < 186 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 800 < PT < 1000 GeV in the central dijet region.
Particle-level distributions of groomed AK8 thrust (charged-only) in 65 < PT < 88 GeV in the forward dijet 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 186 < PT < 254 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 88 < PT < 120 GeV in the central dijet region.
We present an angular analysis of the $B^{+}\rightarrow K^{\ast+}(\rightarrow K_{S}^{0}\pi^{+})\mu^{+}\mu^{-}$ decay using 9$\,\mbox{fb}^{-1}$ of $pp$ collision data collected with the LHCb experiment. For the first time, the full set of CP-averaged angular observables is measured in intervals of the dimuon invariant mass squared. Local deviations from Standard Model predictions are observed, similar to those in previous LHCb analyses of the isospin-partner $B^{0}\rightarrow K^{\ast0}\mu^{+}\mu^{-}$ decay. The global tension is dependent on which effective couplings are considered and on the choice of theory nuisance parameters.
Results for the CP-averaged observables Fl, Afb and S3–S9. The first uncertainties are statistical and the second systematic.
Results for the optimised observables FL and P1–P'8. The first uncertainties are statistical and the second systematic.
The CP-averaged observable Fl versus q2. The first (second) error bars represent the statistical (total) uncertainties.
The CP-averaged observable S3 versus q2. The first (second) error bars represent the statistical (total) uncertainties.
The CP-averaged observable S4 versus q2. The first (second) error bars represent the statistical (total) uncertainties.
The CP-averaged observable S5 versus q2. The first (second) error bars represent the statistical (total) uncertainties.
The CP-averaged observable Afb versus q2. The first (second) error bars represent the statistical (total) uncertainties.
The CP-averaged observable S7 versus q2. The first (second) error bars represent the statistical (total) uncertainties.
The CP-averaged observable S8 versus q2. The first (second) error bars represent the statistical (total) uncertainties.
The CP-averaged observable S9 versus q2. The first (second) error bars represent the statistical (total) uncertainties.
The optimised observable Fl versus q2. The first (second) error bars represent the statistical (total) uncertainties.
The optimised observable P1 versus q2. The first (second) error bars represent the statistical (total) uncertainties.
The optimised observable P2 versus q2. The first (second) error bars represent the statistical (total) uncertainties.
The optimised observable P3 versus q2. The first (second) error bars represent the statistical (total) uncertainties.
The optimised observable P4' versus q2. The first (second) error bars represent the statistical (total) uncertainties.
The optimised observable P5' versus q2. The first (second) error bars represent the statistical (total) uncertainties.
The optimised observable P6' versus q2. The first (second) error bars represent the statistical (total) uncertainties.
The optimised observable P8' versus q2. The first (second) error bars represent the statistical (total) uncertainties.
Correlation matrix for the CP-averaged observables FL, AFB and S3–S9 from the maximum-likelihood fit in the interval 0.10 < q2 < 0.98 GeV2/c4
Correlation matrix for the CP-averaged observables FL, AFB and S3–S9 from the maximum-likelihood fit in the interval 1.10 < q2 < 2.50 GeV2/c4
Correlation matrix for the CP-averaged observables FL, AFB and S3–S9 from the maximum-likelihood fit in the interval 2.50 < q2 < 4.00 GeV2/c4
Correlation matrix for the CP-averaged observables FL, AFB and S3–S9 from the maximum-likelihood fit in the interval 4.00 < q2 < 6.00 GeV2/c4
Correlation matrix for the CP-averaged observables FL, AFB and S3–S9 from the maximum-likelihood fit in the interval 6.00 < q2 < 8.00 GeV2/c4
Correlation matrix for the CP-averaged observables FL, AFB and S3–S9 from the maximum-likelihood fit in the interval 11.00 < q2 < 12.50 GeV2/c4
Correlation matrix for the CP-averaged observables FL, AFB and S3–S9 from the maximum-likelihood fit in the interval 15.00 < q2 < 17.00 GeV2/c4
Correlation matrix for the CP-averaged observables FL, AFB and S3–S9 from the maximum-likelihood fit in the interval 17.00 < q2 < 19.00 GeV2/c4
Correlation matrix for the CP-averaged observables FL, AFB and S3–S9 from the maximum-likelihood fit in the interval 1.10 < q2 < 6.00 GeV2/c4
Correlation matrix for the CP-averaged observables FL, AFB and S3–S9 from the maximum-likelihood fit in the interval 15.00 < q2 < 19.00 GeV2/c4
Correlation matrix for the optimised observables FL and P1–P'8 from the maximum-likelihood fit in the interval 0.10 < q2 < 0.98 GeV2/c4
Correlation matrix for the optimised observables FL and P1–P'8 from the maximum-likelihood fit in the interval 1.10 < q2 < 2.50 GeV2/c4
Correlation matrix for the optimised observables FL and P1–P'8 from the maximum-likelihood fit in the interval 2.50 < q2 < 4.00 GeV2/c4
Correlation matrix for the optimised observables FL and P1–P'8 from the maximum-likelihood fit in the interval 4.00 < q2 < 6.00 GeV2/c4
Correlation matrix for the optimised observables FL and P1–P'8 from the maximum-likelihood fit in the interval 6.00 < q2 < 8.00 GeV2/c4
Correlation matrix for the optimised observables FL and P1–P'8 from the maximum-likelihood fit in the interval 11.00 < q2 < 12.50 GeV2/c4
Correlation matrix for the optimised observables FL and P1–P'8 from the maximum-likelihood fit in the interval 15.00 < q2 < 17.00 GeV2/c4
Correlation matrix for the optimised observables FL and P1–P'8 from the maximum-likelihood fit in the interval 17.00 < q2 < 19.00 GeV2/c4
Correlation matrix for the optimised observables FL and P1–P'8 from the maximum-likelihood fit in the interval 1.10 < q2 < 6.00 GeV2/c4
Correlation matrix for the optimised observables FL and P1–P'8 from the maximum-likelihood fit in the interval 15.00 < q2 < 19.00 GeV2/c4
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.
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.
Measurements of the top quark polarization and top quark pair ($\mathrm{t\bar{t}}$) spin correlations are presented using events containing two oppositely charged leptons (e$^+$e$^-$, e$^\pm\mu^\mp$, or $\mu^+\mu^-$) produced in proton-proton collisions at a center-of-mass energy of 13 TeV. The data were recorded by the CMS experiment at the LHC in 2016 and correspond to an integrated luminosity of 35.9 fb$^{-1}$. A set of parton-level normalized differential cross sections, sensitive to each of the independent coefficients of the spin-dependent parts of the $\mathrm{t\bar{t}}$ production density matrix, is measured for the first time at 13 TeV. The measured distributions and extracted coefficients are compared with standard model predictions from simulations at next-to-leading-order (NLO) accuracy in quantum chromodynamics (QCD), and from NLO QCD calculations including electroweak corrections. All measurements are found to be consistent with the expectations of the standard model. The normalized differential cross sections are used in fits to constrain the anomalous chromomagnetic and chromoelectric dipole moments of the top quark to $-$0.24 $<C_\text{tG}/\Lambda^{2}$ $<$ 0.07 TeV$^{-2}$ and $-$0.33 $< C^{I}_\text{tG}/\Lambda^{2}$ $<$ 0.20 TeV$^{-2}$, respectively, at 95% confidence level.
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.
Energy correlators that describe energy-weighted distances between two or three particles in a jet are measured using an event sample of $\sqrt{s}$ = 13 TeV proton-proton collisions collected by the CMS experiment and corresponding to an integrated luminosity of 36.3 fb$^{-1}$. The measured distributions reveal two key features of the strong interaction: confinement and asymptotic freedom. By comparing the ratio of the two measured distributions with theoretical calculations that resum collinear emissions at approximate next-to-next-to-leading logarithmic accuracy matched to a next-to-leading order calculation, the strong coupling is determined at the Z boson mass: $\alpha_\mathrm{S}(m_\mathrm{Z})$ = 0.1229$^{+0.0040}_{-0.0050}$, the most precise $\alpha_\mathrm{S}(m_\mathrm{Z})$ value obtained using jet substructure observables.
Unfolded E2C distributions in data compared to MC predictions.
Unfolded E2C distributions in data compared to MC predictions.
Unfolded E2C distributions in data compared to MC predictions.
Unfolded E2C distributions in data compared to MC predictions.
Unfolded E2C distributions in data compared to MC predictions.
Unfolded E2C distributions in data compared to MC predictions.
Unfolded E2C distributions in data compared to MC predictions.
Unfolded E2C distributions in data compared to MC predictions.
Unfolded E3C distributions in data compared to MC predictions.
Unfolded E3C distributions in data compared to MC predictions.
Unfolded E3C distributions in data compared to MC predictions.
Unfolded E3C distributions in data compared to MC predictions.
Unfolded E3C distributions in data compared to MC predictions.
Unfolded E3C distributions in data compared to MC predictions.
Unfolded E3C distributions in data compared to MC predictions.
Unfolded E3C distributions in data compared to MC predictions.
Unfolded E3C/E2C distributions in data compared to NLO+NNLL_approx predictions. Theoretial uncertainty in each bin is handled fully correlated as shape uncertainty. For the one-sided uncertainties, we symmetrize them when performing the fit.
Unfolded E3C/E2C distributions in data compared to NLO+NNLL_approx predictions. Theoretial uncertainty in each bin is handled fully correlated as shape uncertainty. For the one-sided uncertainties, we symmetrize them when performing the fit.
Unfolded E3C/E2C distributions in data compared to NLO+NNLL_approx predictions. Theoretial uncertainty in each bin is handled fully correlated as shape uncertainty. For the one-sided uncertainties, we symmetrize them when performing the fit.
Unfolded E3C/E2C distributions in data compared to NLO+NNLL_approx predictions. Theoretial uncertainty in each bin is handled fully correlated as shape uncertainty. For the one-sided uncertainties, we symmetrize them when performing the fit.
Unfolded E3C/E2C distributions in data compared to NLO+NNLL_approx predictions. Theoretial uncertainty in each bin is handled fully correlated as shape uncertainty. For the one-sided uncertainties, we symmetrize them when performing the fit.
Unfolded E3C/E2C distributions in data compared to NLO+NNLL_approx predictions. Theoretial uncertainty in each bin is handled fully correlated as shape uncertainty. For the one-sided uncertainties, we symmetrize them when performing the fit.
Unfolded E3C/E2C distributions in data compared to NLO+NNLL_approx predictions. Theoretial uncertainty in each bin is handled fully correlated as shape uncertainty. For the one-sided uncertainties, we symmetrize them when performing the fit.
Unfolded E3C/E2C distributions in data compared to NLO+NNLL_approx predictions. Theoretial uncertainty in each bin is handled fully correlated as shape uncertainty. For the one-sided uncertainties, we symmetrize them when performing the fit.
The fitted slopes of the E3C/E2C data distributions as a function of jet pt are used to illustrate the dependency of alphas on jet pt.
Unfolded E3C/E2C distributions in data compared to MC predictions.
Unfolded E3C/E2C distributions in data compared to MC predictions.
Unfolded E3C/E2C distributions in data compared to MC predictions.
Unfolded E3C/E2C distributions in data compared to MC predictions.
Unfolded E3C/E2C distributions in data compared to MC predictions.
Unfolded E3C/E2C distributions in data compared to MC predictions.
Unfolded E3C/E2C distributions in data compared to MC predictions.
Unfolded E3C/E2C distributions in data compared to MC predictions.
The chi2 scan result using eq.3 for different alphas.
The correlation matrix is composed by 10 jet pt region, each region is represented by a block in the plot. Inside each block, there are 22 xL bins same as the E2C, E3C and E3C/E2C distributions. Therefore, the x and y bins of the correlation matrix is given by, binNumber = pT_index * 22 + xL_index.
The correlation matrix is composed by 10 jet pt region, each region is represented by a block in the plot. Inside each block, there are 22 xL bins same as the E2C, E3C and E3C/E2C distributions. Therefore, the x and y bins of the correlation matrix is given by, binNumber = pT_index * 22 + xL_index.
The correlation matrix is composed by 10 jet pt region, each region is represented by a block in the plot. Inside each block, there are 22 xL bins same as the E2C, E3C and E3C/E2C distributions. Therefore, the x and y bins of the correlation matrix is given by, binNumber = pT_index * 22 + xL_index.
The energy weight of E2C as defined in eq.1 in the paper is used in the unfolding, the binning is listed in this table.
The energy weight of E3C as defined in eq.1 in the paper is used in the unfolding, the binning is listed in this table.
An angular analysis of the $B^{0}\rightarrow K^{*0}(\rightarrow K^{+}\pi^{-})\mu^{+}\mu^{-}$ decay is presented. The dataset corresponds to an integrated luminosity of $3.0\,{\mbox{fb}^{-1}}$ of $pp$ collision data collected at the LHCb experiment. The complete angular information from the decay is used to determine $C\!P$-averaged observables and $C\!P$ asymmetries, taking account of possible contamination from decays with the $K^{+}\pi^{-}$ system in an S-wave configuration. The angular observables and their correlations are reported in bins of $q^2$, the invariant mass squared of the dimuon system. The observables are determined both from an unbinned maximum likelihood fit and by using the principal moments of the angular distribution. In addition, by fitting for $q^2$-dependent decay amplitudes in the region $1.1<q^{2}<6.0\mathrm{\,Ge\kern -0.1em V}^{2}/c^{4}$, the zero-crossing points of several angular observables are computed. A global fit is performed to the complete set of $C\!P$-averaged observables obtained from the maximum likelihood fit. This fit indicates differences with predictions based on the Standard Model at the level of 3.4 standard deviations. These differences could be explained by contributions from physics beyond the Standard Model, or by an unexpectedly large hadronic effect that is not accounted for in the Standard Model predictions.
CP-averaged angular observables evaluated by the unbinned maximum likelihood fit.
CP-averaged angular observables evaluated by the unbinned maximum likelihood fit. The first uncertainties are statistical and the second systematic.
CP-asymmetric angular observables evaluated by the unbinned maximum likelihood fit. The first uncertainties are statistical and the second systematic.
Optimised angular observables evaluated by the unbinned maximum likelihood fit. The first uncertainties are statistical and the second systematic.
CP-averaged angular observables evaluated using the method of moments. The first uncertainties are statistical and the second systematic.
Optimised observables evaluated using the method of moments. The first uncertainties are statistical and the second systematic.
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