Showing 10 of 1901 results
Heavy-flavour hadron production provides information about the transport properties and microscopic structure of the quark-gluon plasma created in ultra-relativistic heavy-ion collisions. A measurement of the muons from semileptonic decays of charm and bottom hadrons produced in Pb+Pb and $pp$ collisions at a nucleon-nucleon centre-of-mass energy of 5.02 TeV with the ATLAS detector at the Large Hadron Collider is presented. The Pb+Pb data were collected in 2015 and 2018 with sampled integrated luminosities of $208~\mathrm{\mu b}^{-1}$ and $38~\mathrm{\mu b^{-1}}$, respectively, and $pp$ data with a sampled integrated luminosity of $1.17~\mathrm{pb}^{-1}$ were collected in 2017. Muons from heavy-flavour semileptonic decays are separated from the light-flavour hadronic background using the momentum imbalance between the inner detector and muon spectrometer measurements, and muons originating from charm and bottom decays are further separated via the muon track's transverse impact parameter. Differential yields in Pb+Pb collisions and differential cross sections in $pp$ collisions for such muons are measured as a function of muon transverse momentum from 4 GeV to 30 GeV in the absolute pseudorapidity interval $|\eta| < 2$. Nuclear modification factors for charm and bottom muons are presented as a function of muon transverse momentum in intervals of Pb+Pb collision centrality. The measured nuclear modification factors quantify a significant suppression of the yields of muons from decays of charm and bottom hadrons, with stronger effects for muons from charm hadron decays.
A search for new heavy resonances decaying to pairs of bosons (WW, WZ, or WH) is presented. The analysis uses data from proton-proton collisions collected with the CMS detector at a center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of 137 fb$^{-1}$. One of the bosons is required to be a W boson decaying to an electron or muon and a neutrino, while the other boson is required to be reconstructed as a single jet with mass and substructure compatible with a quark pair from a W, Z, or Higgs boson decay. The search is performed in the resonance mass range between 1.0 and 4.5 TeV and includes a specific search for resonances produced via vector boson fusion. The signal is extracted using a two-dimensional maximum likelihood fit to the jet mass and the diboson invariant mass distributions. No significant excess is observed above the estimated background. Model-independent upper limits on the production cross sections of spin-0, spin-1, and spin-2 heavy resonances are derived as functions of the resonance mass and are interpreted in the context of bulk radion, heavy vector triplet, and bulk graviton models. The reported bounds are the most stringent to date.
Exclusion limits on the product of the production cross section and the branching fraction for a Bulk Graviton produced by gluon fusion and decaying to WW, as a function of the resonance mass hypothesis.
Exclusion limits on the product of the production cross section and the branching fraction for a Bulk Graviton produced by vector boson fusion and decaying to WW, as a function of the resonance mass hypothesis.
Exclusion limits on the product of the production cross section and the branching fraction for a Radion produced by gluon fusion and decaying to WW, as a function of the resonance mass hypothesis.
Exclusion limits on the product of the production cross section and the branching fraction for a Radion produced by vector boson fusion and decaying to WW, as a function of the resonance mass hypothesis.
Exclusion limits on the product of the production cross section and the branching fraction for a Z' produced by quark annihilation and decaying to WW, as a function of the resonance mass hypothesis.
Exclusion limits on the product of the production cross section and the branching fraction for a Z' produced by vector boson fusion and decaying to WW, as a function of the resonance mass hypothesis.
Exclusion limits on the product of the production cross section and the branching fraction for a W' produced by quark annihilation and decaying to WZ, as a function of the resonance mass hypothesis.
Exclusion limits on the product of the production cross section and the branching fraction for a W' produced by vector boson fusion and decaying to WZ, as a function of the resonance mass hypothesis.
Exclusion limits on the product of the production cross section and the branching fraction for a W' produced by quark annihilation and decaying to WH, as a function of the resonance mass hypothesis.
Measurements of the inclusive and differential fiducial cross sections of the Higgs boson are presented, using the $\tau$ lepton decay channel. The differential cross sections are measured as functions of the Higgs boson transverse momentum, jet multiplicity, and transverse momentum of the leading jet in the event if any. The analysis is performed using proton-proton data collected with the CMS detector at the LHC at a center-of-mass energy of 13 TeV and corresponding to an integrated luminosity of 138 fb$^{-1}$. These are the first differential measurements of the Higgs boson cross section in the final state of two $\tau$ leptons, and they constitute a significant improvement over measurements in other final states in events with a large jet multiplicity or with a Lorentz-boosted Higgs boson.
The fiducial differential signal strength and cross section in each Higgs pT bin. Both the unregularized and regularized signal strengths are given; they do not include uncertainties in the SM signal normalization. The fiducial cross section and its full uncertainty in each bin are also given. The last bin is inclusive.
The fiducial differential signal strength and cross section in each jet multiplicity bin. Both the unregularized and regularized signal strengths are given; they do not include uncertainties in the SM signal normalization. The fiducial cross section and its full uncertainty in each bin are also given. The last bin is inclusive.
The fiducial differential signal strength and cross section in each leading jet pT bin. Both the unregularized and regularized signal strengths are given; they do not include uncertainties in the SM signal normalization. The fiducial cross section and its full uncertainty in each bin are also given. The last bin is inclusive.
The correlation matrix for the Higgs pT measurements, both for the unregularized and regularized fits. The last bin is inclusive.
The correlation matrix for the jet multiplicity measurements, both for the unregularized and regularized fits. The last bin is inclusive.
The correlation matrix for the leading jet pT measurements, both for the unregularized and regularized fits. The last bin is inclusive.
The fiducial integrated signal strength and cross section.
A search is presented for lepton-flavor violating decays of the Higgs boson to $\mu\tau$ and e$\tau$. The data set corresponds to an integrated luminosity of 137 fb$^{-1}$ collected at the LHC in proton-proton collisions at a center-of-mass energy of 13 TeV. No significant excess has been found, and the results are interpreted in terms of upper limits on lepton-flavor violating branching fractions of the Higgs boson. The observed (expected) upper limits on the branching fractions are, respectively, $\mathcal{B}($H $\to\mu\tau)$$\lt$ 0.15 (0.15)% and $\mathcal{B}($H$\to$e$\tau)$ $\lt$ 0.22 (0.16)% at 95% confidence level.
Observed (expected) 95% CL upper limits on $B(H\to\mu\tau)$ for each individual category and combined
Observed (expected) 95% CL upper limits on $B(H\to e\tau)$ for each individual category and combined
Summary of observed and expected upper limits at 95% CL, best fit branching fractions and corresponding constraints on Yukawa couplings for the $H\to\mu\tau$ and $H\to e\tau$ channels
95% CL observed upper limits on the Yukawa couplings
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.
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 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 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 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 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 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 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 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 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 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 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 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 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.
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 186 < PT < 254 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 254 < PT < 326 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 326 < PT < 408 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 408 < PT < 1500 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 50 < PT < 65 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 65 < PT < 88 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 88 < PT < 120 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 120 < PT < 150 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 150 < PT < 186 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 186 < PT < 254 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 254 < PT < 326 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 326 < PT < 408 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 408 < PT < 481 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 481 < PT < 614 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 614 < PT < 800 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 800 < PT < 1000 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 1000 < PT < 4000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 50 < PT < 65 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 65 < PT < 88 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 88 < PT < 120 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 120 < PT < 150 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 150 < PT < 186 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 186 < PT < 254 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 254 < PT < 326 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 326 < PT < 408 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 408 < PT < 481 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 481 < PT < 614 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 800 < PT < 1000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 1000 < PT < 4000 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 50 < PT < 65 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 65 < PT < 88 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 88 < PT < 120 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 120 < PT < 150 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 150 < PT < 186 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 186 < PT < 254 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 254 < PT < 326 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 326 < PT < 408 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 408 < PT < 481 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 481 < PT < 614 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 614 < PT < 800 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 800 < PT < 1000 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 1000 < PT < 4000 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 50 < PT < 65 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 88 < PT < 120 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 120 < PT < 150 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 150 < PT < 186 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 186 < PT < 254 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 254 < PT < 326 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 326 < PT < 408 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 408 < PT < 1500 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust (charged-only) in 50 < PT < 65 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust (charged-only) in 65 < PT < 88 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust (charged-only) in 88 < PT < 120 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust (charged-only) in 120 < PT < 150 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust (charged-only) in 150 < PT < 186 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust (charged-only) in 186 < PT < 254 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust (charged-only) in 254 < PT < 326 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust (charged-only) in 326 < PT < 408 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust (charged-only) in 408 < PT < 1500 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 50 < PT < 65 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 65 < PT < 88 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 88 < PT < 120 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 120 < PT < 150 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 150 < PT < 186 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 186 < PT < 254 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 254 < PT < 326 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 326 < PT < 408 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 408 < PT < 481 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 481 < PT < 614 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 614 < PT < 800 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 800 < PT < 1000 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 1000 < PT < 4000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust (charged-only) in 65 < PT < 88 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust (charged-only) in 88 < PT < 120 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust (charged-only) in 120 < PT < 150 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust (charged-only) in 150 < PT < 186 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust (charged-only) in 186 < PT < 254 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust (charged-only) in 254 < PT < 326 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust (charged-only) in 326 < PT < 408 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust (charged-only) in 408 < PT < 481 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust (charged-only) in 481 < PT < 614 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust (charged-only) in 614 < PT < 800 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust (charged-only) in 800 < PT < 1000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust (charged-only) in 1000 < PT < 4000 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 65 < PT < 88 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 88 < PT < 120 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 120 < PT < 150 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 150 < PT < 186 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 186 < PT < 254 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 254 < PT < 326 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 408 < PT < 481 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 481 < PT < 614 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 614 < PT < 800 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 800 < PT < 1000 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 1000 < PT < 4000 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 50 < PT < 65 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 65 < PT < 88 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 88 < PT < 120 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 120 < PT < 150 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 150 < PT < 186 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 186 < PT < 254 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 254 < PT < 326 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 326 < PT < 408 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 408 < PT < 1500 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width (charged-only) in 50 < PT < 65 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width (charged-only) in 65 < PT < 88 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width (charged-only) in 120 < PT < 150 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width (charged-only) in 150 < PT < 186 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width (charged-only) in 186 < PT < 254 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width (charged-only) in 254 < PT < 326 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width (charged-only) in 326 < PT < 408 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width (charged-only) in 408 < PT < 1500 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 50 < PT < 65 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 65 < PT < 88 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 88 < PT < 120 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 120 < PT < 150 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 150 < PT < 186 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 186 < PT < 254 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 254 < PT < 326 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 326 < PT < 408 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 408 < PT < 481 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 481 < PT < 614 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 614 < PT < 800 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 800 < PT < 1000 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 1000 < PT < 4000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width (charged-only) in 50 < PT < 65 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width (charged-only) in 88 < PT < 120 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width (charged-only) in 120 < PT < 150 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width (charged-only) in 150 < PT < 186 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width (charged-only) in 186 < PT < 254 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width (charged-only) in 254 < PT < 326 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width (charged-only) in 326 < PT < 408 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width (charged-only) in 408 < PT < 481 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width (charged-only) in 481 < PT < 614 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width (charged-only) in 614 < PT < 800 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width (charged-only) in 800 < PT < 1000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width (charged-only) in 1000 < PT < 4000 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 50 < PT < 65 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 65 < PT < 88 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 88 < PT < 120 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 120 < PT < 150 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 150 < PT < 186 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 186 < PT < 254 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 254 < PT < 326 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 326 < PT < 408 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 408 < PT < 481 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 481 < PT < 614 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 614 < PT < 800 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 800 < PT < 1000 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 1000 < PT < 4000 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 multiplicity in 50 < PT < 65 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 multiplicity in 65 < PT < 88 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 multiplicity in 150 < PT < 186 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 multiplicity in 186 < PT < 254 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 multiplicity in 254 < PT < 326 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 multiplicity in 326 < PT < 408 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 multiplicity in 408 < PT < 1500 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity in 50 < PT < 65 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity in 65 < PT < 88 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity in 88 < PT < 120 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity in 120 < PT < 150 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity in 150 < PT < 186 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity in 186 < PT < 254 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity in 254 < PT < 326 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity in 326 < PT < 408 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 multiplicity in 50 < PT < 65 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 multiplicity in 65 < PT < 88 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 multiplicity in 88 < PT < 120 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 multiplicity in 150 < PT < 186 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 multiplicity in 186 < PT < 254 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 multiplicity in 254 < PT < 326 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 multiplicity in 326 < PT < 408 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 multiplicity in 408 < PT < 481 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 multiplicity in 481 < PT < 614 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 multiplicity in 614 < PT < 800 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 multiplicity in 800 < PT < 1000 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 multiplicity in 1000 < PT < 4000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity in 50 < PT < 65 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity in 65 < PT < 88 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity in 88 < PT < 120 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity in 120 < PT < 150 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity in 150 < PT < 186 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity in 186 < PT < 254 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity in 254 < PT < 326 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity in 326 < PT < 408 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity in 408 < PT < 481 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity in 481 < PT < 614 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity in 614 < PT < 800 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity in 800 < PT < 1000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity in 1000 < PT < 4000 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 multiplicity in 50 < PT < 65 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 multiplicity in 65 < PT < 88 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 multiplicity in 88 < PT < 120 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 multiplicity in 120 < PT < 150 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 multiplicity in 150 < PT < 186 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 multiplicity in 186 < PT < 254 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 multiplicity in 254 < PT < 326 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 multiplicity in 326 < PT < 408 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 multiplicity in 408 < PT < 481 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 multiplicity in 614 < PT < 800 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 multiplicity in 800 < PT < 1000 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 multiplicity in 1000 < PT < 4000 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 pTD2 in 50 < PT < 65 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 pTD2 in 65 < PT < 88 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 pTD2 in 88 < PT < 120 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 pTD2 in 150 < PT < 186 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 pTD2 in 186 < PT < 254 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 pTD2 in 254 < PT < 326 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 pTD2 in 326 < PT < 408 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 pTD2 in 408 < PT < 1500 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 in 50 < PT < 65 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 in 88 < PT < 120 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 in 120 < PT < 150 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 in 150 < PT < 186 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 in 186 < PT < 254 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 in 254 < PT < 326 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 in 326 < PT < 408 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 pTD2 in 50 < PT < 65 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 pTD2 in 65 < PT < 88 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 pTD2 in 88 < PT < 120 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 pTD2 in 150 < PT < 186 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 pTD2 in 186 < PT < 254 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 pTD2 in 254 < PT < 326 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 pTD2 in 326 < PT < 408 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 pTD2 in 408 < PT < 481 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 pTD2 in 481 < PT < 614 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 pTD2 in 614 < PT < 800 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 pTD2 in 800 < PT < 1000 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 pTD2 in 1000 < PT < 4000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 in 50 < PT < 65 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 in 65 < PT < 88 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 in 88 < PT < 120 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 in 120 < PT < 150 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 in 150 < PT < 186 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 in 186 < PT < 254 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 in 254 < PT < 326 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 in 326 < PT < 408 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 in 408 < PT < 481 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 in 481 < PT < 614 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 in 614 < PT < 800 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 in 800 < PT < 1000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 in 1000 < PT < 4000 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 pTD2 in 50 < PT < 65 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 pTD2 in 65 < PT < 88 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 pTD2 in 88 < PT < 120 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 pTD2 in 120 < PT < 150 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 pTD2 in 150 < PT < 186 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 pTD2 in 186 < PT < 254 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 pTD2 in 254 < PT < 326 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 pTD2 in 408 < PT < 481 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 pTD2 in 481 < PT < 614 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 pTD2 in 614 < PT < 800 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 pTD2 in 800 < PT < 1000 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 pTD2 in 1000 < PT < 4000 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 thrust in 50 < PT < 65 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 thrust in 65 < PT < 88 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 thrust in 88 < PT < 120 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 thrust in 150 < PT < 186 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 thrust in 186 < PT < 254 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 thrust in 254 < PT < 326 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 thrust in 326 < PT < 408 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 thrust in 408 < PT < 1500 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust in 50 < PT < 65 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust in 65 < PT < 88 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust in 88 < PT < 120 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust in 150 < PT < 186 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust in 186 < PT < 254 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust in 254 < PT < 326 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust in 326 < PT < 408 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust in 408 < PT < 1500 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 thrust in 50 < PT < 65 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 thrust in 65 < PT < 88 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 thrust in 88 < PT < 120 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 thrust in 150 < PT < 186 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 thrust in 186 < PT < 254 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 thrust in 254 < PT < 326 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 thrust in 326 < PT < 408 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 thrust in 408 < PT < 481 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 thrust in 481 < PT < 614 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 thrust in 614 < PT < 800 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 thrust in 800 < PT < 1000 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 thrust in 1000 < PT < 4000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust in 50 < PT < 65 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust in 65 < PT < 88 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust in 88 < PT < 120 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust in 120 < PT < 150 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust in 150 < PT < 186 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust in 186 < PT < 254 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust in 254 < PT < 326 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust in 326 < PT < 408 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust in 408 < PT < 481 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust in 481 < PT < 614 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust in 614 < PT < 800 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust in 800 < PT < 1000 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 thrust in 50 < PT < 65 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 thrust in 65 < PT < 88 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 thrust in 88 < PT < 120 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 thrust in 120 < PT < 150 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 thrust in 150 < PT < 186 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 thrust in 186 < PT < 254 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 thrust in 254 < PT < 326 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 thrust in 326 < PT < 408 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 thrust in 408 < PT < 481 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 thrust in 481 < PT < 614 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 thrust in 614 < PT < 800 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 thrust in 800 < PT < 1000 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 thrust in 1000 < PT < 4000 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 width in 50 < PT < 65 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 width in 65 < PT < 88 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 width in 88 < PT < 120 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 width in 150 < PT < 186 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 width in 186 < PT < 254 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 width in 254 < PT < 326 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 width in 326 < PT < 408 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 width in 408 < PT < 1500 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width in 50 < PT < 65 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width in 65 < PT < 88 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width in 88 < PT < 120 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width in 120 < PT < 150 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width in 150 < PT < 186 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width in 186 < PT < 254 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width in 254 < PT < 326 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width in 326 < PT < 408 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 width in 50 < PT < 65 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 width in 65 < PT < 88 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 width in 88 < PT < 120 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 width in 150 < PT < 186 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 width in 186 < PT < 254 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 width in 254 < PT < 326 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 width in 326 < PT < 408 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 width in 408 < PT < 481 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 width in 481 < PT < 614 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 width in 614 < PT < 800 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 width in 800 < PT < 1000 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 width in 1000 < PT < 4000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width in 50 < PT < 65 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width in 65 < PT < 88 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width in 88 < PT < 120 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width in 120 < PT < 150 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width in 150 < PT < 186 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width in 186 < PT < 254 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width in 254 < PT < 326 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width in 326 < PT < 408 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width in 408 < PT < 481 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width in 481 < PT < 614 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width in 614 < PT < 800 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width in 800 < PT < 1000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width in 1000 < PT < 4000 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 width in 50 < PT < 65 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 width in 88 < PT < 120 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 width in 120 < PT < 150 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 width in 186 < PT < 254 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 width in 254 < PT < 326 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 width in 326 < PT < 408 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 width in 408 < PT < 481 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 width in 481 < PT < 614 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 width in 614 < PT < 800 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 width in 800 < PT < 1000 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 width in 1000 < PT < 4000 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 LHA in 50 < PT < 65 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 LHA in 65 < PT < 88 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 LHA in 88 < PT < 120 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 LHA in 150 < PT < 186 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 LHA in 186 < PT < 254 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 LHA in 254 < PT < 326 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 LHA in 326 < PT < 408 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 LHA in 408 < PT < 1500 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA in 50 < PT < 65 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA in 65 < PT < 88 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA in 88 < PT < 120 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA in 120 < PT < 150 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA in 150 < PT < 186 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA in 186 < PT < 254 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA in 254 < PT < 326 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA in 326 < PT < 408 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA in 408 < PT < 1500 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 LHA in 65 < PT < 88 GeV in the central dijet region.
Particle-level distributions of groomed AK4 LHA in 88 < PT < 120 GeV in the central dijet region.
Particle-level distributions of groomed AK4 LHA in 150 < PT < 186 GeV in the central dijet region.
Particle-level distributions of groomed AK4 LHA in 186 < PT < 254 GeV in the central dijet region.
Particle-level distributions of groomed AK4 LHA in 254 < PT < 326 GeV in the central dijet region.
Particle-level distributions of groomed AK4 LHA in 326 < PT < 408 GeV in the central dijet region.
Particle-level distributions of groomed AK4 LHA in 408 < PT < 481 GeV in the central dijet region.
Particle-level distributions of groomed AK4 LHA in 481 < PT < 614 GeV in the central dijet region.
Particle-level distributions of groomed AK4 LHA in 614 < PT < 800 GeV in the central dijet region.
Particle-level distributions of groomed AK4 LHA in 800 < PT < 1000 GeV in the central dijet region.
Particle-level distributions of groomed AK4 LHA in 1000 < PT < 4000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA in 50 < PT < 65 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA in 65 < PT < 88 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA in 88 < PT < 120 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA in 186 < PT < 254 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA in 254 < PT < 326 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA in 326 < PT < 408 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA in 408 < PT < 481 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA in 481 < PT < 614 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA in 614 < PT < 800 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA in 800 < PT < 1000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA in 1000 < PT < 4000 GeV in the central dijet region.
Particle-level distributions of groomed AK4 LHA in 50 < PT < 65 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 LHA in 65 < PT < 88 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 LHA in 88 < PT < 120 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 LHA in 120 < PT < 150 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 LHA in 150 < PT < 186 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 LHA in 186 < PT < 254 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 LHA in 254 < PT < 326 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 LHA in 326 < PT < 408 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 LHA in 408 < PT < 481 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 LHA in 481 < PT < 614 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 LHA in 614 < PT < 800 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 LHA in 800 < PT < 1000 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 LHA in 1000 < PT < 4000 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 50 < PT < 65 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 65 < PT < 88 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 88 < PT < 120 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 120 < PT < 150 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 150 < PT < 186 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 186 < PT < 254 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 254 < PT < 326 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 326 < PT < 408 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 408 < PT < 1500 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA (charged-only) in 50 < PT < 65 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA (charged-only) in 65 < PT < 88 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA (charged-only) in 88 < PT < 120 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA (charged-only) in 120 < PT < 150 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA (charged-only) in 150 < PT < 186 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA (charged-only) in 186 < PT < 254 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA (charged-only) in 254 < PT < 326 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA (charged-only) in 326 < PT < 408 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA (charged-only) in 408 < PT < 1500 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 50 < PT < 65 GeV in the central dijet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 88 < PT < 120 GeV in the central dijet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 120 < PT < 150 GeV in the central dijet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 150 < PT < 186 GeV in the central dijet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 186 < PT < 254 GeV in the central dijet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 254 < PT < 326 GeV in the central dijet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 326 < PT < 408 GeV in the central dijet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 408 < PT < 481 GeV in the central dijet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 481 < PT < 614 GeV in the central dijet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 614 < PT < 800 GeV in the central dijet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 800 < PT < 1000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA (charged-only) in 50 < PT < 65 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA (charged-only) in 65 < PT < 88 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA (charged-only) in 88 < PT < 120 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA (charged-only) in 120 < PT < 150 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA (charged-only) in 150 < PT < 186 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA (charged-only) in 186 < PT < 254 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA (charged-only) in 254 < PT < 326 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA (charged-only) in 326 < PT < 408 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA (charged-only) in 408 < PT < 481 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA (charged-only) in 481 < PT < 614 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA (charged-only) in 614 < PT < 800 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA (charged-only) in 800 < PT < 1000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA (charged-only) in 1000 < PT < 4000 GeV in the central dijet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 50 < PT < 65 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 65 < PT < 88 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 88 < PT < 120 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 120 < PT < 150 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 150 < PT < 186 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 186 < PT < 254 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 254 < PT < 326 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 326 < PT < 408 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 408 < PT < 481 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 481 < PT < 614 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 614 < PT < 800 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 800 < PT < 1000 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 1000 < PT < 4000 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 50 < PT < 65 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 65 < PT < 88 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 88 < PT < 120 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 120 < PT < 150 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 150 < PT < 186 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 186 < PT < 254 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 254 < PT < 326 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 326 < PT < 408 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 408 < PT < 1500 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity (charged-only) in 50 < PT < 65 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity (charged-only) in 65 < PT < 88 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity (charged-only) in 88 < PT < 120 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity (charged-only) in 120 < PT < 150 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity (charged-only) in 150 < PT < 186 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity (charged-only) in 186 < PT < 254 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity (charged-only) in 254 < PT < 326 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity (charged-only) in 326 < PT < 408 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity (charged-only) in 408 < PT < 1500 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 50 < PT < 65 GeV in the central dijet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 65 < PT < 88 GeV in the central dijet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 88 < PT < 120 GeV in the central dijet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 120 < PT < 150 GeV in the central dijet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 186 < PT < 254 GeV in the central dijet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 254 < PT < 326 GeV in the central dijet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 326 < PT < 408 GeV in the central dijet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 408 < PT < 481 GeV in the central dijet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 481 < PT < 614 GeV in the central dijet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 614 < PT < 800 GeV in the central dijet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 800 < PT < 1000 GeV in the central dijet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 1000 < PT < 4000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity (charged-only) in 50 < PT < 65 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity (charged-only) in 65 < PT < 88 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity (charged-only) in 88 < PT < 120 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity (charged-only) in 120 < PT < 150 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity (charged-only) in 186 < PT < 254 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity (charged-only) in 254 < PT < 326 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity (charged-only) in 326 < PT < 408 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity (charged-only) in 408 < PT < 481 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity (charged-only) in 481 < PT < 614 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity (charged-only) in 614 < PT < 800 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity (charged-only) in 800 < PT < 1000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity (charged-only) in 1000 < PT < 4000 GeV in the central dijet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 50 < PT < 65 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 65 < PT < 88 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 88 < PT < 120 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 120 < PT < 150 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 150 < PT < 186 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 186 < PT < 254 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 254 < PT < 326 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 326 < PT < 408 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 408 < PT < 481 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 481 < PT < 614 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 614 < PT < 800 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 800 < PT < 1000 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 1000 < PT < 4000 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 pTD2 (charged-only) in 50 < PT < 65 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 pTD2 (charged-only) in 65 < PT < 88 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 pTD2 (charged-only) in 88 < PT < 120 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 pTD2 (charged-only) in 120 < PT < 150 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 pTD2 (charged-only) in 150 < PT < 186 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 pTD2 (charged-only) in 186 < PT < 254 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 pTD2 (charged-only) in 254 < PT < 326 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 pTD2 (charged-only) in 408 < PT < 1500 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 (charged-only) in 50 < PT < 65 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 (charged-only) in 65 < PT < 88 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 (charged-only) in 88 < PT < 120 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 (charged-only) in 120 < PT < 150 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 (charged-only) in 150 < PT < 186 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 (charged-only) in 186 < PT < 254 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 (charged-only) in 254 < PT < 326 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 (charged-only) in 326 < PT < 408 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 (charged-only) in 408 < PT < 1500 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 pTD2 (charged-only) in 50 < PT < 65 GeV in the central dijet region.
Particle-level distributions of groomed AK4 pTD2 (charged-only) in 65 < PT < 88 GeV in the central dijet region.
Particle-level distributions of groomed AK4 pTD2 (charged-only) in 88 < PT < 120 GeV in the central dijet region.
Particle-level distributions of groomed AK4 pTD2 (charged-only) in 120 < PT < 150 GeV in the central dijet region.
Particle-level distributions of groomed AK4 pTD2 (charged-only) in 150 < PT < 186 GeV in the central dijet region.
Particle-level distributions of groomed AK4 pTD2 (charged-only) in 186 < PT < 254 GeV in the central dijet region.
Particle-level distributions of groomed AK4 pTD2 (charged-only) in 254 < PT < 326 GeV in the central dijet region.
Particle-level distributions of groomed AK4 pTD2 (charged-only) in 326 < PT < 408 GeV in the central dijet region.
Particle-level distributions of groomed AK4 pTD2 (charged-only) in 408 < PT < 481 GeV in the central dijet region.
Particle-level distributions of groomed AK4 pTD2 (charged-only) in 481 < PT < 614 GeV in the central dijet region.
Particle-level distributions of groomed AK4 pTD2 (charged-only) in 614 < PT < 800 GeV in the central dijet region.
Particle-level distributions of groomed AK4 pTD2 (charged-only) in 800 < PT < 1000 GeV in the central dijet region.
Particle-level distributions of groomed AK4 pTD2 (charged-only) in 1000 < PT < 4000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 (charged-only) in 50 < PT < 65 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 (charged-only) in 65 < PT < 88 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 (charged-only) in 88 < PT < 120 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 (charged-only) in 120 < PT < 150 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 (charged-only) in 150 < PT < 186 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 (charged-only) in 186 < PT < 254 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 (charged-only) in 254 < PT < 326 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 (charged-only) in 326 < PT < 408 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 (charged-only) in 408 < PT < 481 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 (charged-only) in 481 < PT < 614 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 (charged-only) in 614 < PT < 800 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 (charged-only) in 800 < PT < 1000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 (charged-only) in 1000 < PT < 4000 GeV in the central dijet region.
Particle-level distributions of groomed AK4 pTD2 (charged-only) in 50 < PT < 65 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 pTD2 (charged-only) in 65 < PT < 88 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 pTD2 (charged-only) in 88 < PT < 120 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 pTD2 (charged-only) in 120 < PT < 150 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 pTD2 (charged-only) in 150 < PT < 186 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 pTD2 (charged-only) in 186 < PT < 254 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 pTD2 (charged-only) in 254 < PT < 326 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 pTD2 (charged-only) in 326 < PT < 408 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 pTD2 (charged-only) in 408 < PT < 481 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 pTD2 (charged-only) in 481 < PT < 614 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 pTD2 (charged-only) in 614 < PT < 800 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 pTD2 (charged-only) in 800 < PT < 1000 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 pTD2 (charged-only) in 1000 < PT < 4000 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 thrust (charged-only) in 65 < PT < 88 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 thrust (charged-only) in 88 < PT < 120 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 thrust (charged-only) in 120 < PT < 150 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 thrust (charged-only) in 150 < PT < 186 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 thrust (charged-only) in 186 < PT < 254 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 thrust (charged-only) in 254 < PT < 326 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 thrust (charged-only) in 326 < PT < 408 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 thrust (charged-only) in 408 < PT < 1500 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 thrust (charged-only) in 50 < PT < 65 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 thrust (charged-only) in 65 < PT < 88 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 thrust (charged-only) in 120 < PT < 150 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 thrust (charged-only) in 150 < PT < 186 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 thrust (charged-only) in 186 < PT < 254 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 thrust (charged-only) in 254 < PT < 326 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 thrust (charged-only) in 326 < PT < 408 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 thrust (charged-only) in 408 < PT < 1500 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 thrust (charged-only) in 50 < PT < 65 GeV in the central dijet region.
Particle-level distributions of groomed AK4 thrust (charged-only) in 65 < PT < 88 GeV in the central dijet region.
Particle-level distributions of groomed AK4 thrust (charged-only) in 88 < PT < 120 GeV in the central dijet region.
Particle-level distributions of groomed AK4 thrust (charged-only) in 120 < PT < 150 GeV in the central dijet region.
Particle-level distributions of groomed AK4 thrust (charged-only) in 150 < PT < 186 GeV in the central dijet region.
Particle-level distributions of groomed AK4 thrust (charged-only) in 186 < PT < 254 GeV in the central dijet region.
Particle-level distributions of groomed AK4 thrust (charged-only) in 254 < PT < 326 GeV in the central dijet region.
Particle-level distributions of groomed AK4 thrust (charged-only) in 326 < PT < 408 GeV in the central dijet region.
Particle-level distributions of groomed AK4 thrust (charged-only) in 408 < PT < 481 GeV in the central dijet region.
This paper presents a measurement of the electroweak production of two jets in association with a $Z\gamma$ pair, with the $Z$ boson decaying into two neutrinos. It also presents a search for invisible or partially invisible decays of a Higgs boson with a mass of 125 GeV produced through vector-boson fusion with a photon in the final state. These results use data from LHC proton-proton collisions at $\sqrt{s}$ = 13 TeV collected with the ATLAS detector and corresponding to an integrated luminosity of 139 fb$^{-1}$. The event signature, shared by all benchmark processes considered for the measurements and searches, is characterized by a significant amount of unbalanced transverse momentum and a photon in the final state, in addition to a pair of forward jets. Electroweak $Z\gamma$ production in association with two jets is observed in this final state with a significance of 5.2 (5.1 expected) standard deviations. The measured fiducial cross-section for this process is 1.31$\pm$0.29 fb. An observed (expected) upper limit of 0.37 ($0.34^{+0.15}_{-0.10}$) at 95% confidence level is set on the branching ratio of a 125 GeV Higgs boson to invisible particles, assuming the Standard Model production cross-section. The signature is also interpreted in the context of decays of a Higgs boson into a photon and a dark photon. An observed (expected) 95% CL upper limit on the branching ratio for this decay is set at 0.018 ($0.017^{+0.007}_{-0.005}$), assuming the Standard Model production cross-section for a 125 GeV Higgs boson.
Post-fit results for all $m_\text{jj}$ SR and CR bins in the EW $Z \gamma + \text{jets}$ cross-section measurement with the $\mu_{Z \gamma_\text{EW}}$ signal normalization floating. The post-fit uncertainties include statistical, experimental, and theory contributions.
Post-fit results for all DNN SR and CR bins in the search for $H \to \text{inv.}$ with the $\mathcal{B}_\text{inv}$ signal normalization set to zero. For the $Z_\text{Rev.Cen.}^\gamma$ CR, the third bin contains all events with DNN output score values of 0.6-1.0. The $H \to \text{inv.}$ signal is scaled to a $\mathcal{B}_\text{inv}$ of 37%. The post-fit uncertainties include statistical, experimental, and theoretical contributions.
Post-fit results for the ten [$m_\text{jj}$, $m_\text{T}$] bins constituting the SR and CRs defined for the dark photon search with the $\mathcal{B}(H \to \gamma \gamma_\text{d})$ signal normalization set to zero. A $H \to \gamma \gamma_\text{d}$ signal is shown for two different mass hypotheses (125 GeV, 500 GeV) and scaled to a branching ratio of 2% and 1%, respectively. The post-fit uncertainties include statistical, experimental, and theoretical contributions.
Post-fit $m_\text{T}(\gamma, E_\text{T}^\text{miss})$ distribution in the inclusive signal region for the dark-photon search with the 125 GeV mass $\mathcal{B}(H \to \gamma \gamma_\text{d})$ signal normalization set to zero. A $H \to \gamma \gamma_\text{d}$ decay signal is shown for two different mass hypotheses, 125 GeV and 500 GeV, and scaled to a $\mathcal{B}(H \to \gamma \gamma_\text{d})$ of 2% and 1%, respectively. Events with $m_\text{T}(\gamma, E_\text{T}^\text{miss})$ larger than the rightmost bin boundary are added to that bin.
The 95% CL upper limit on the Higgs boson production cross-section times branching ratio to $\gamma \gamma_\text{d}$ is shown for different VBF-produced scalar-mediator-mass hypotheses in the NWA. The theoretically predicted cross-section of a Higgs boson produced via VBF and with the $\mathcal{B}(H \to \gamma \gamma_\text{d}) =$ 5% is superimposed on the $\pm 1\sigma$ and $\pm 2\sigma$ NNLO QCD + NLO EW uncertainty band of the expected production cross-section limit.
Post-fit $m_\text{jj}$ distribution in the inclusive signal region. The Higgs boson invisible decay signal is scaled to a $\mathcal{B}_\text{inv}$ of 37%. Events with $m_\text{jj}$ larger than the rightmost bin boundary are added to that bin.
Post-fit $m_\text{jj}$ distribution in the one-lepton control region $W_{\ell \nu}^\gamma$ CR. Events with $m_\text{jj}$ larger than the rightmost bin boundary are added to that bin.
Post-fit $m_\text{T}$ distribution in the one lepton control region. Events with $m_\text{T}$ larger than the rightmost bin boundary are added to that bin.
Post-fit photon centrality distribution in the zero lepton signal plus control region with the $\mathcal{B}_\text{inv}$ signal normalization set to zero in the fit.
Post-fit photon $E_\text{T}$ distribution in the zero lepton signal region with the $\mathcal{B}_\text{inv}$ signal normalization set to zero in the fit.
Post-fit photon centrality distribution in the zero lepton signal plus control region resulting from the fit to the $m_\text{jj}$ distribution for EW $Z \gamma + \text{jets}$. The post-fit uncertainties include statistical, experimental, and theory contributions.
Post-fit photon $E_\text{T}$ distribution in the zero lepton signal region resulting from the fit to the $m_\text{jj}$ distribution for EW $Z \gamma + \text{jets}$. The post-fit uncertainties include statistical, experimental, and theory contributions.
Post-fit DNN output score distribution in the one lepton control region.
Yields for the EW $Z \gamma + \text{jets}$ process are shown after each selection along with relative and absolute signal acceptance efficiencies.
Yields for the 125 GeV Higgs boson with $\mathcal{B}_\text{inv.} =$ 1 signal produced by the vector boson fusion process in association with a final state photon are shown after each selection along with relative and absolute signal acceptance efficiencies.
Yields for the 125 GeV Higgs boson with $\mathcal{B}(H \to \gamma \gamma_\text{d}) =$ 1 signal produced by the vector boson fusion process are shown after each selection along with relative and absolute signal acceptance efficiencies.
A search for the exotic decay of the Higgs boson ($H$) into a $b\bar{b}$ resonance plus missing transverse momentum is described. The search is performed with the ATLAS detector at the Large Hadron Collider using 139 $\mathrm{fb}^{-1}$ of $pp$ collisions at $\sqrt{s} = 13$ TeV. The search targets events from $ZH$ production in an NMSSM scenario where $H \rightarrow \tilde{\chi}^{0}_{2}\tilde{\chi}^{0}_{1}$, with $\tilde{\chi}^{0}_{2} \rightarrow {a} \tilde{\chi}^{0}_{1}$, where $a$ is a light pseudoscalar Higgs boson and $\tilde{\chi}^{0}_{1,2}$ are the two lightest neutralinos. The decay of the $a$ boson into a pair of $b$-quarks results in a peak in the dijet invariant mass distribution. The final-state signature consists of two leptons, two or more jets, at least one of which is identified as originating from a $b$-quark, and missing transverse momentum. Observations are consistent with Standard Model expectations and upper limits are set on the product of cross section times branching ratio for a three-dimensional scan of the masses of the $\tilde{\chi}^{0}_{2}$, $\tilde{\chi}^{0}_{1}$ and $a$ boson.
Distribution of the dijet invariant mass in CRZ. The Z+HF and $t\bar{t}$ scale factors, described in the text, have been applied to the simulated samples. The distribution labeled "Signal" is for the model with ($m_a$, $m_{\tilde{\chi}_{1}^{0}}$, $m_{\tilde{\chi}_{2}^{0}}$) = (45 GeV, 10 GeV, 80 GeV).
Distribution of the missing transverse energy in VRMET. The Z+HF and $t\bar{t}$ scale factors, described in the text, have been applied to the simulated samples. The distribution labeled "Signal" is for the model with ($m_a$, $m_{\tilde{\chi}_{1}^{0}}$, $m_{\tilde{\chi}_{2}^{0}}$) = (45 GeV, 10 GeV, 80 GeV).
Distribution of the dijet invariant mass in CRTop. The Z+HF and $t\bar{t}$ scale factors, described in the text, have been applied to the simulated samples. The distribution labeled "Signal" is for the model with ($m_a$, $m_{\tilde{\chi}_{1}^{0}}$, $m_{\tilde{\chi}_{2}^{0}}$) = (45 GeV, 10 GeV, 80 GeV).
Distribution of the missing transverse energy in CRTop. The Z+HF and $t\bar{t}$ scale factors, described in the text, have been applied to the simulated samples. The distribution labeled "Signal" is for the model with ($m_a$, $m_{\tilde{\chi}_{1}^{0}}$, $m_{\tilde{\chi}_{2}^{0}}$) = (45 GeV, 10 GeV, 80 GeV).
Distribution of the dijet invariant mass in the signal region, shown together with the parameterized background model (labelled "Bkg Model"). For reference, the MC prediction for the SM background is also shown (labelled "SM MC"). The Z+HF and $t\bar{t}$ scale factors, described in the text, have been applied to the simulated samples. The signal region is defined to have dijet invariant mass > 20 GeV. The distribution labeled "Signal" is for the model with ($m_a$, $m_{\tilde{\chi}_{1}^{0}}$, $m_{\tilde{\chi}_{2}^{0}}$) = (45 GeV, 10 GeV, 80 GeV).
Upper limits at 95% CL on the $pp \rightarrow ZH$ cross section times the branching ratio for $Z \rightarrow \ell^{+}\ell^{-}$ (where $\ell = e, \mu \;\mathrm{or}\; \tau$) and $H \rightarrow \tilde{\chi}_{2}^{0}\tilde{\chi}_{1}^{0} \rightarrow a \tilde{\chi}_{1}^{0}\tilde{\chi}_{1}^{0} \rightarrow b\bar{b} \tilde{\chi}_{1}^{0}\tilde{\chi}_{1}^{0}$ as a function of $m_{a}$ for $m_{\tilde{\chi}_{1}^{0}} = 10$ GeV and $m_{\tilde{\chi}_{2}^{0}} = 65$ GeV in the NMSSM scenario described in the text. All branching ratios in the Higgs boson decay chain after the decay $H \rightarrow \tilde{\chi}_{2}^{0}\tilde{\chi}_{1}^{0}$ are set to 100%.
Upper limits at 95% CL on the $pp \rightarrow ZH$ cross section times the branching ratio for $Z \rightarrow \ell^{+}\ell^{-}$ (where $\ell = e, \mu \;\mathrm{or}\; \tau$) and $H \rightarrow \tilde{\chi}_{2}^{0}\tilde{\chi}_{1}^{0} \rightarrow a \tilde{\chi}_{1}^{0}\tilde{\chi}_{1}^{0} \rightarrow b\bar{b} \tilde{\chi}_{1}^{0}\tilde{\chi}_{1}^{0}$ as a function of $m_{a}$ for $m_{\tilde{\chi}_{1}^{0}} = 10$ GeV and $m_{\tilde{\chi}_{2}^{0}} = 80$ GeV in the NMSSM scenario described in the text. All branching ratios in the Higgs boson decay chain after the decay $H \rightarrow \tilde{\chi}_{2}^{0}\tilde{\chi}_{1}^{0}$ are set to 100%.
Upper limits at 95% CL on the $pp \rightarrow ZH$ cross section times the branching ratio for $Z \rightarrow \ell^{+}\ell^{-}$ (where $\ell = e, \mu\; \mathrm{or}\; \tau$) and $H \rightarrow \tilde{\chi}_{2}^{0}\tilde{\chi}_{1}^{0} \rightarrow a \tilde{\chi}_{1}^{0}\tilde{\chi}_{1}^{0} \rightarrow b\bar{b} \tilde{\chi}_{1}^{0}\tilde{\chi}_{1}^{0}$ as a function of $m_{a}$ for $m_{\tilde{\chi}_{1}^{0}} = 10$ GeV and $m_{\tilde{\chi}_{2}^{0}} = 95$ GeV in the NMSSM scenario described in the text. All branching ratios in the Higgs boson decay chain after the decay $H \rightarrow \tilde{\chi}_{2}^{0}\tilde{\chi}_{1}^{0}$ are set to 100%.
Upper limits at 95% CL on the $pp \rightarrow ZH$ cross section times the branching ratio for $Z \rightarrow \ell^{+}\ell^{-}$ (where $\ell = e, \mu\; \mathrm{or}\; \tau$) and $H \rightarrow \tilde{\chi}_{2}^{0}\tilde{\chi}_{1}^{0} \rightarrow a \tilde{\chi}_{1}^{0}\tilde{\chi}_{1}^{0} \rightarrow b\bar{b} \tilde{\chi}_{1}^{0}\tilde{\chi}_{1}^{0}$ as a function of $m_{a}$ for $m_{\tilde{\chi}_{1}^{0}} = 10$ GeV and $m_{\tilde{\chi}_{2}^{0}} = 110$ GeV in the NMSSM scenario described in the text. All branching ratios in the Higgs boson decay chain after the decay $H \rightarrow \tilde{\chi}_{2}^{0}\tilde{\chi}_{1}^{0}$ are set to 100%.
Upper limits at 95% CL on the $pp \rightarrow ZH$ cross section times the branching ratio for $Z \rightarrow \ell^{+}\ell^{-}$ (where $\ell = e, \mu\; \mathrm{or}\; \tau$) and $H \rightarrow \tilde{\chi}_{2}^{0}\tilde{\chi}_{1}^{0} \rightarrow a \tilde{\chi}_{1}^{0}\tilde{\chi}_{1}^{0} \rightarrow b\bar{b} \tilde{\chi}_{1}^{0}\tilde{\chi}_{1}^{0}$ as a function of $m_{a}$ for $m_{\tilde{\chi}_{1}^{0}} = 20$ GeV and $m_{\tilde{\chi}_{2}^{0}} = 80$ GeV in the NMSSM scenario described in the text. All branching ratios in the Higgs boson decay chain after the decay $H \rightarrow \tilde{\chi}_{2}^{0}\tilde{\chi}_{1}^{0}$ are set to 100%.
Upper limits at 95% CL on the $pp \rightarrow ZH$ cross section times the branching ratio for $Z \rightarrow \ell^{+}\ell^{-}$ (where $\ell = e, \mu \;\mathrm{or}\; \tau$) and $H \rightarrow \tilde{\chi}_{2}^{0}\tilde{\chi}_{1}^{0} \rightarrow a \tilde{\chi}_{1}^{0}\tilde{\chi}_{1}^{0} \rightarrow b\bar{b} \tilde{\chi}_{1}^{0}\tilde{\chi}_{1}^{0}$ as a function of $m_{a}$ for $m_{\tilde{\chi}_{1}^{0}} = 30$ GeV and $m_{\tilde{\chi}_{2}^{0}} = 80$ GeV in the NMSSM scenario described in the text. All branching ratios in the Higgs boson decay chain after the decay $H \rightarrow \tilde{\chi}_{2}^{0}\tilde{\chi}_{1}^{0}$ are set to 100%.
Upper limits at 95% CL on the branching ratio $H \rightarrow \tilde{\chi}_{2}^{0}\tilde{\chi}_{1}^{0} \rightarrow a \tilde{\chi}_{1}^{0}\tilde{\chi}_{1}^{0} \rightarrow b\bar{b} \tilde{\chi}_{1}^{0}\tilde{\chi}_{1}^{0}$ as a function of $m_{a}$ for $m_{\tilde{\chi}_{1}^{0}} = 10$ GeV and $m_{\tilde{\chi}_{2}^{0}} = 65$ GeV in the NMSSM scenario described in the text. The SM $ZH$ cross section is assumed.
Upper limits at 95% CL on the branching ratio $H \rightarrow \tilde{\chi}_{2}^{0}\tilde{\chi}_{1}^{0} \rightarrow a \tilde{\chi}_{1}^{0}\tilde{\chi}_{1}^{0} \rightarrow b\bar{b} \tilde{\chi}_{1}^{0}\tilde{\chi}_{1}^{0}$ as a function of $m_{a}$ for $m_{\tilde{\chi}_{1}^{0}} = 10$ GeV and $m_{\tilde{\chi}_{2}^{0}} = 80$ GeV in the NMSSM scenario described in the text. The SM $ZH$ cross section is assumed.
Upper limits at 95% CL on the branching ratio $H \rightarrow \tilde{\chi}_{2}^{0}\tilde{\chi}_{1}^{0} \rightarrow a \tilde{\chi}_{1}^{0}\tilde{\chi}_{1}^{0} \rightarrow b\bar{b} \tilde{\chi}_{1}^{0}\tilde{\chi}_{1}^{0}$ as a function of $m_{a}$ for $m_{\tilde{\chi}_{1}^{0}} = 10$ GeV and $m_{\tilde{\chi}_{2}^{0}} = 95$ GeV in the NMSSM scenario described in the text. The SM $ZH$ cross section is assumed.
Upper limits at 95% CL on the branching ratio $H \rightarrow \tilde{\chi}_{2}^{0}\tilde{\chi}_{1}^{0} \rightarrow a \tilde{\chi}_{1}^{0}\tilde{\chi}_{1}^{0} \rightarrow b\bar{b} \tilde{\chi}_{1}^{0}\tilde{\chi}_{1}^{0}$ as a function of $m_{a}$ for $m_{\tilde{\chi}_{1}^{0}} = 10$ GeV and $m_{\tilde{\chi}_{2}^{0}} = 110$ GeV in the NMSSM scenario described in the text. The SM $ZH$ cross section is assumed.
Upper limits at 95% CL on the branching ratio $H \rightarrow \tilde{\chi}_{2}^{0}\tilde{\chi}_{1}^{0} \rightarrow a \tilde{\chi}_{1}^{0}\tilde{\chi}_{1}^{0} \rightarrow b\bar{b} \tilde{\chi}_{1}^{0}\tilde{\chi}_{1}^{0}$ as a function of $m_{a}$ for $m_{\tilde{\chi}_{1}^{0}} = 20$ GeV and $m_{\tilde{\chi}_{2}^{0}} = 80$ GeV in the NMSSM scenario described in the text. The SM $ZH$ cross section is assumed.
Upper limits at 95% CL on the branching ratio $H \rightarrow \tilde{\chi}_{2}^{0}\tilde{\chi}_{1}^{0} \rightarrow a \tilde{\chi}_{1}^{0}\tilde{\chi}_{1}^{0} \rightarrow b\bar{b} \tilde{\chi}_{1}^{0}\tilde{\chi}_{1}^{0}$ as a function of $m_{a}$ for $m_{\tilde{\chi}_{1}^{0}} = 30$ GeV and $m_{\tilde{\chi}_{2}^{0}} = 80$ GeV in the NMSSM scenario described in the text. The SM $ZH$ cross section is assumed.
Unweighted and weighted number of events after each stage of selection for the NMSSM scenario with $pp \rightarrow ZH$, $Z \rightarrow \ell^{+}\ell^{-}$, $H \rightarrow \tilde{\chi}_{2}^{0}\tilde{\chi}_{1}^{0} \rightarrow a \tilde{\chi}_{1}^{0}\tilde{\chi}_{1}^{0} \rightarrow b\bar{b} \tilde{\chi}_{1}^{0}\tilde{\chi}_{1}^{0}$ where $(m_{a}, m_{\tilde{\chi}_{1}^{0}}, m_{\tilde{\chi}_{2}^{0}}) = (45,10,80)$ GeV and the Z boson decaying to $e^{+}e^{-}, \;\mu^{+}\mu^{-} \;\mathrm{or}\; \tau^{+}\tau^{-}$. All branching ratios in the Higgs boson decay chain are set to 100%. The weighted number of events corresponds to an integrated luminosity of $139 \;\mathrm{fb}^{-1}$. The "skimming selection" required either a single electron or muon with $p_{T} > 100\;$ GeV or a pair of electrons or muons each with $p_{T} > 20\;$ GeV. The preselection requirements include the trigger, absence of a bad jet or bad muon, and two leptons, where a lepton is either an electron or a muon.
Acceptance and efficiency of this analysis for the signal models considered in this paper. The signal is an NMSSM scenario with $pp \rightarrow ZH$, $Z \rightarrow \ell^{+}\ell^{-}$, $H \rightarrow \tilde{\chi}_{2}^{0}\tilde{\chi}_{1}^{0} \rightarrow a \tilde{\chi}_{1}^{0}\tilde{\chi}_{1}^{0} \rightarrow b\bar{b} \tilde{\chi}_{1}^{0}\tilde{\chi}_{1}^{0}$ where the values of $(m_{a}, m_{\tilde{\chi}_{1}^{0}}, m_{\tilde{\chi}_{2}^{0}})$ are varied. The Z boson decays to $e^{+}e^{-}, \mu^{+}\mu^{-} \;\mathrm{or}\; \tau^{+}\tau^{-}$. All branching ratios in the Higgs boson decay chain are set to 100%. The product of acceptance times efficiency is defined by the fraction of simulated events that pass all the selection criteria of this analysis. The acceptance is defined by the fraction of simulated events that pass all the selection criteria as applied to Monte Carlo truth-level quantities. The efficiency is then defined as the acceptance times efficiency, divided by the acceptance.
Acceptance and efficiency of this analysis for the signal models considered in this paper. The signal is an NMSSM scenario with $pp \rightarrow ZH$, $Z \rightarrow \ell^{+}\ell^{-}$, $H \rightarrow \tilde{\chi}_{2}^{0}\tilde{\chi}_{1}^{0} \rightarrow a \tilde{\chi}_{1}^{0}\tilde{\chi}_{1}^{0} \rightarrow b\bar{b} \tilde{\chi}_{1}^{0}\tilde{\chi}_{1}^{0}$ where the values of $(m_{a}, m_{\tilde{\chi}_{1}^{0}}, m_{\tilde{\chi}_{2}^{0}})$ are varied. The Z boson decays to $e^{+}e^{-}, \mu^{+}\mu^{-} \;\mathrm{or}\; \tau^{+}\tau^{-}$. All branching ratios in the Higgs boson decay chain are set to 100%. The product of acceptance times efficiency is defined by the fraction of simulated events that pass all the selection criteria of this analysis. The acceptance is defined by the fraction of simulated events that pass all the selection criteria as applied to Monte Carlo truth-level quantities. The efficiency is then defined as the acceptance times efficiency, divided by the acceptance.
A search is presented for a heavy vector resonance decaying into a Z boson and the standard model Higgs boson, where the Z boson is identified through its leptonic decays to electrons, muons, or neutrinos, and the Higgs boson is identified through its hadronic decays. The search is performed in a Lorentz-boosted regime and is based on data collected from 2016 to 2018 at the CERN LHC, corresponding to an integrated luminosity of 137 fb$^{-1}$. Upper limits are derived on the production of a narrow heavy resonance Z', and a mass below 3.5 and 3.7 TeV is excluded at 95% confidence level in models where the heavy vector boson couples exclusively to fermions and to bosons, respectively. These are the most stringent limits placed on the Heavy Vector Triplet Z' model to date. If the heavy vector boson couples exclusively to standard model bosons, upper limits on the product of the cross section and branching fraction are set between 23 and 0.3 fb for a Z' mass between 0.8 and 4.6 TeV, respectively. This is the first limit set on a heavy vector boson coupling exclusively to standard model bosons in its production and decay.
The product of signal acceptance and efficiency in the 0l categories for the signal produced via qqbar annihilation.
The product of signal acceptance and efficiency in the 2l categories for the signal produced via qqbar annihilation.
The product of signal acceptance and efficiency in the 0l categories for the signal produced via vector boson fusion.
The product of signal acceptance and efficiency in the 2l categories for the signal produced via vector boson fusion.
$m_{X}^{T}$ distribution in data in the 0l 2b non-VBF category. The data is shown as Events/10 GeV. The distribution is shown up 4000 GeV, which corresponds to the event with the highest $m_{X}^{T}$ observed in the SR.
$m_{X}^{T}$ distribution in data in the 0l $\leq$1b non-VBF category. The data is shown as Events/10 GeV. The distribution is shown up 4000 GeV, which corresponds to the event with the highest $m_{X}^{T}$ observed in the SR.
$m_{X}$ distribution in data in the 2e 2b non-VBF category. The data is shown as Events/10 GeV. The distribution is shown up 4000 GeV, which corresponds to the event with the highest $m_{X}$ observed in the SR.
$m_{X}$ distribution in data in the 2e $\leq$1b non-VBF category. The data is shown as Events/10 GeV. The distribution is shown up 4000 GeV, which corresponds to the event with the highest $m_{X}$ observed in the SR.
$m_{X}$ distribution in data in the 2$\mu$ 2b non-VBF category. The data is shown as Events/10 GeV. The distribution is shown up 4000 GeV, which corresponds to the event with the highest $m_{X}$ observed in the SR.
$m_{X}$ distribution in data in the 2$\mu$ $\leq$1b non-VBF category. The data is shown as Events/10 GeV. The distribution is shown up 4000 GeV, which corresponds to the event with the highest $m_{X}$ observed in the SR.
$m_{X}^{T}$ distribution in data in the 0l 2b VBF category. The data is shown as Events/10 GeV. The distribution is shown up 4000 GeV, which corresponds to the event with the highest $m_{X}^{T}$ observed in the SR.
$m_{X}^{T}$ distribution in data in the 0l $\leq$1b VBF category. The data is shown as Events/10 GeV. The distribution is shown up 4000 GeV, which corresponds to the event with the highest $m_{X}^{T}$ observed in the SR.
$m_{X}$ distribution in data in the 2e 2b VBF category. The data is shown as Events/10 GeV. The distribution is shown up 4000 GeV, which corresponds to the event with the highest $m_{X}$ observed in the SR.
$m_{X}$ distribution in data in the 2e $\leq$1b VBF category. The data is shown as Events/10 GeV. The distribution is shown up 4000 GeV, which corresponds to the event with the highest $m_{X}$ observed in the SR.
$m_{X}$ distribution in data in the 2$\mu$ 2b VBF category. The data is shown as Events/10 GeV. The distribution is shown up 4000 GeV, which corresponds to the event with the highest $m_{X}$ observed in the SR.
$m_{X}$ distribution in data in the 2$\mu$ $\leq$1b VBF category. The data is shown as Events/10 GeV. The distribution is shown up 4000 GeV, which corresponds to the event with the highest $m_{X}$ observed in the SR.
Observed and expected 95% CL upper limit on $\sigma \mathcal{B}$(Z'-> ZH) with all categories combined for the non-VBF signal, including all statistical and systematic uncertainties. The inner green band and the outer yellow band indicate the regions containing 68 and 95%, respectively, of the distribution of expected limits under the background-only hypothesis. The CMS search for a heavy resonance using 2016 data and the same final state [JHEP 11 (2018) 172] is shown as a comparison.
Observed and expected 95% CL upper limit on $\sigma \mathcal{B}$(Z'-> ZH) with all categories combined for the VBF signal, including all statistical and systematic uncertainties. The inner green band and the outer yellow band indicate the regions containing 68 and 95%, respectively, of the distribution of expected limits under the background-only hypothesis.
Observed exclusion limit in the space of the HVT model parameters [$g_{V}c_{H}$, $g^{2}c_{F}/g_{V}$] for mass hypotheses of 2 TeV for the non-VBF signal.
Observed exclusion limit in the space of the HVT model parameters [$g_{V}c_{H}$, $g^{2}c_{F}/g_{V}$] for mass hypotheses of 3 TeV for the non-VBF signal.
Observed exclusion limit in the space of the HVT model parameters [$g_{V}c_{H}$, $g^{2}c_{F}/g_{V}$] for mass hypotheses of 4 TeV for the non-VBF signal.
The ALICE Collaboration reports the first fully-corrected measurements of the $N$-subjettiness observable for track-based jets in heavy-ion collisions. This study is performed using data recorded in pp and Pb$-$Pb collisions at centre-of-mass energies of $\sqrt{s} = 7$ TeV and $\sqrt{s_{\rm NN}} = 2.76$ TeV, respectively. In particular the ratio of 2-subjettiness to 1-subjettiness, $\tau_{2}/\tau_{1}$, which is sensitive to the rate of two-pronged jet substructure, is presented. Energy loss of jets traversing the strongly interacting medium in heavy-ion collisions is expected to change the rate of two-pronged substructure relative to vacuum. The results are presented for jets with a resolution parameter of $R = 0.4$ and charged jet transverse momentum of $40 \leq p_{\rm T,\rm jet} \leq 60$ GeV/$c$, which constitute a larger jet resolution and lower jet transverse momentum interval than previous measurements in heavy-ion collisions. This has been achieved by utilising a semi-inclusive hadron-jet coincidence technique to suppress the larger jet combinatorial background in this kinematic region. No significant modification of the $\tau_{2}/\tau_{1}$ observable for track-based jets in Pb--Pb collisions is observed relative to vacuum PYTHIA6 and PYTHIA8 references at the same collision energy. The measurements of $\tau_{2}/\tau_{1}$, together with the splitting aperture angle $\Delta R$, are also performed in pp collisions at $\sqrt{s}=7$ TeV for inclusive jets. These results are compared with PYTHIA calculations at $\sqrt{s}=7$ TeV, in order to validate the model as a vacuum reference for the Pb$-$Pb centre-of-mass energy. The PYTHIA references for $\tau_{2}/\tau_{1}$ are shifted to larger values compared to the measurement in pp collisions. This hints at a reduction in the rate of two-pronged jets in Pb--Pb collisions compared to pp collisions.
The transverse momentum ($p_\mathrm{T}$) distributions of $\Lambda$, $\Xi^-$, and $\Omega^-$ baryons, their antiparticles, and K$^0_\mathrm{S}$ mesons are measured in proton-proton (pp) and proton-lead (pPb) collisions at a nucleon-nucleon center-of-mass energy of 5.02 TeV over a broad rapidity range. The data, corresponding to integrated luminosities of 40.2 nb$^{-1}$ and 15.6 $\mu$b$^{-1}$ for pp and pPb collisions, respectively, were collected by the CMS experiment. The nuclear modification factor $R_\mathrm{pPb}$, defined as the ratio of the particle yield in pPb collisions and a scaled pp reference, is measured for each particle. A strong dependence on particle species is observed in the $p_\mathrm{T}$ range from 2 to 7 GeV, where $R_\mathrm{pPb}$ for K$^0_\mathrm{S}$ is consistent with unity, while an enhancement ordered by strangeness content and/or particle mass is observed for the three baryons. In pPb collisions, the strange hadron production is asymmetric about the nucleon-nucleon center-of-mass rapidity. Enhancements, which depend on the particle type, are observed in the direction of the Pb beam. The results are compared to predictions from EPOS LHC, which includes parametrized radial flow. The model is in qualitative agreement with the $R_\mathrm{pPb}$ data, but fails to describe the dependence on particle species in the yield asymmetries measured away from mid-rapidity in pPb collisions.
Invariant $p_{T}$-differential spectra of ${K_{0}}^{S}$ in p+p and p+Pb at $\sqrt{s}$=5.02 TeV in various |$y_{CM}$| ranges
Invariant $p_{T}$-differential spectra of ${K_{0}}^{S}$ in p+p and p+Pb at $\sqrt{s}$=5.02 TeV in various $y_{CM}$ ranges
Invariant $p_{T}$-differential spectra of $\Lambda + \bar{\Lambda}$ in p+p and p+Pb at $\sqrt{s}$=5.02 TeV in various |$y_{CM}$| ranges
Invariant $p_{T}$-differential spectra of $\Lambda + \bar{\Lambda}$ in p+p and p+Pb at $\sqrt{s}$=5.02 TeV in various $y_{CM}$ ranges
Invariant $p_{T}$-differential spectra of $\Xi- + \bar{\Xi+}$ in p+p and p+Pb at $\sqrt{s}$=5.02 TeV in various |$y_{CM}$| ranges
Invariant $p_{T}$-differential spectra of $\Xi- + \bar{\Xi+}$ in p+p and p+Pb at $\sqrt{s}$=5.02 TeV in various $y_{CM}$ ranges
Invariant $p_{T}$-differential spectra of $\Omega- + \bar{\Omega+}$ in p+p and p+Pb at $\sqrt{s}$=5.02 TeV in |$y_{CM}$| < 1.8
Invariant $p_{T}$-differential spectra of $\Omega- + \bar{\Omega+}$ in p+p and p+Pb at $\sqrt{s}$=5.02 TeV in |$y_{CM}$| < 1.8
$R_{pPb}$ in p+Pb at $\sqrt{s}$=5.02 TeV in |$y_{CM}$| < 1.8
$R_{pPb}$ in p+Pb at $\sqrt{s}$=5.02 TeV in |$y_{CM}$| < 1.8
$R_{pPb}$ in p+Pb at $\sqrt{s}$=5.02 TeV in -1.8 < $y_{CM}$ < 0
$R_{pPb}$ in p+Pb at $\sqrt{s}$=5.02 TeV in |$y_{CM}$| < 1.8
$R_{pPb}$ in p+Pb at $\sqrt{s}$=5.02 TeV in 0 < $y_{CM}$ < 1.8
$R_{pPb}$ in p+Pb at $\sqrt{s}$=5.02 TeV in |$y_{CM}$| < 1.8
Invariant $p_{T}$-differential spectra of ${K_{0}}^{S}$ in p+Pb at $\sqrt{s}$=5.02 TeV in various $y_{CM}$ ranges
$R_{pPb}$ in p+Pb at $\sqrt{s}$=5.02 TeV in |$y_{CM}$| < 1.8
Invariant $p_{T}$-differential spectra of $\Lambda + \bar{\Lambda}$ in p+Pb at $\sqrt{s}$=5.02 TeV in various $y_{CM}$ ranges
$R_{pPb}$ in p+Pb at $\sqrt{s}$=5.02 TeV in -1.8 < $y_{CM}$ < 0
$Y_{asym}$ in p+Pb at $\sqrt{s}$=5.02 TeV in 0.3 < $y_{CM}$ < 0.8
$R_{pPb}$ in p+Pb at $\sqrt{s}$=5.02 TeV in -1.8 < $y_{CM}$ < 0
$Y_{asym}$ in p+Pb at $\sqrt{s}$=5.02 TeV in 0.8 < $y_{CM}$ < 1.3
$R_{pPb}$ in p+Pb at $\sqrt{s}$=5.02 TeV in -1.8 < $y_{CM}$ < 0
$Y_{asym}$ in p+Pb at $\sqrt{s}$=5.02 TeV in 1.3 < $y_{CM}$ < 1.8
$R_{pPb}$ in p+Pb at $\sqrt{s}$=5.02 TeV in 0 < $y_{CM}$ < 1.8
$R_{pPb}$ in p+Pb at $\sqrt{s}$=5.02 TeV in 0 < $y_{CM}$ < 1.8
$R_{pPb}$ in p+Pb at $\sqrt{s}$=5.02 TeV in 0 < $y_{CM}$ < 1.8
Invariant $p_{T}$-differential spectra of ${K_{0}}^{S}$ in p+Pb at $\sqrt{s}$=5.02 TeV in various $y_{CM}$ ranges
Invariant $p_{T}$-differential spectra of $\Lambda + \bar{\Lambda}$ in p+Pb at $\sqrt{s}$=5.02 TeV in various $y_{CM}$ ranges
$Y_{asym}$ in p+Pb at $\sqrt{s}$=5.02 TeV in 0.3 < |$y_{CM}$| < 0.8
$Y_{asym}$ in p+Pb at $\sqrt{s}$=5.02 TeV in 0.3 < |$y_{CM}$| < 0.8
$Y_{asym}$ in p+Pb at $\sqrt{s}$=5.02 TeV in 0.3 < |$y_{CM}$| < 0.8
$Y_{asym}$ in p+Pb at $\sqrt{s}$=5.02 TeV in 0.8 < |$y_{CM}$| < 1.3
$Y_{asym}$ in p+Pb at $\sqrt{s}$=5.02 TeV in 0.8 < |$y_{CM}$| < 1.3
$Y_{asym}$ in p+Pb at $\sqrt{s}$=5.02 TeV in 0.8 < |$y_{CM}$| < 1.3
$Y_{asym}$ in p+Pb at $\sqrt{s}$=5.02 TeV in 1.3 < |$y_{CM}$| < 1.8
$Y_{asym}$ in p+Pb at $\sqrt{s}$=5.02 TeV in 1.3 < |$y_{CM}$| < 1.8
$Y_{asym}$ in p+Pb at $\sqrt{s}$=5.02 TeV in 1.3 < |$y_{CM}$| < 1.8
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