Showing 10 of 580 results
Measurements of jet substructure describing the composition of quark- and gluon-initiated jets are presented. Proton-proton (pp) collision data at $\sqrt{s}$ =13 TeV collected with the CMS detector are used, corresponding to an integrated luminosity of 35.9 fb$^{-1}$. Generalized angularities are measured that characterize the jet substructure and distinguish quark- and gluon-initiated jets. These observables are sensitive to the distributions of transverse momenta and angular distances within a jet. The analysis is performed using a data sample of dijet events enriched in gluon-initiated jets, and, for the first time, a Z+jet event sample enriched in quark-initiated jets. The observables are measured in bins of jet transverse momentum, and as a function of the jet radius parameter. Each measurement is repeated applying a "soft drop" grooming procedure that removes soft and large angle radiation from the jet. Using these measurements, the ability of various models to describe jet substructure is assessed, showing a clear need for improvements in Monte Carlo generators.
Particle-level distributions of ungroomed AK4 multiplicity in 120 < PT < 150 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 multiplicity in 120 < PT < 150 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 pTD2 in 120 < PT < 150 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 pTD2 in 120 < PT < 150 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 width in 120 < PT < 150 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 LHA in 120 < PT < 150 GeV in the Z+jet region.
Mean of ungroomed LHA (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 forward dijet region.
Mean of ungroomed thrust (charged-only) for AK4 jets as a function of PT in the central dijet region.
Mean of ungroomed multiplicity for AK4 jets as a function of PT in the forward dijet region.
Mean of groomed multiplicity (charged-only) for AK4 jets as a function of PT in the Z+jet region.
Mean of groomed pTD2 (charged-only) for AK4 jets as a function of PT in the Z+jet region.
Mean of groomed thrust (charged-only) for AK4 jets as a function of PT in the Z+jet region.
Mean of ungroomed multiplicity for AK8 jets as a function of PT in the Z+jet region.
Mean of groomed multiplicity for AK8 jets as a function of PT in the Z+jet region.
Particle-level distributions of ungroomed AK4 LHA (charged-only) in 65 < PT < 88 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 186 < PT < 254 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 50 < PT < 65 GeV in the central dijet region.
Correlation matrix of the 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 pTD2 (charged-only) in 150 < PT < 186 GeV in the Z+jet 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.
Particle-level distributions of groomed AK4 thrust (charged-only) in 481 < PT < 614 GeV in the central dijet region.
Particle-level distributions of groomed AK4 thrust (charged-only) in 614 < PT < 800 GeV in the central dijet region.
Particle-level distributions of groomed AK4 thrust (charged-only) in 800 < PT < 1000 GeV in the central dijet region.
Particle-level distributions of groomed AK4 thrust (charged-only) in 1000 < PT < 4000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 thrust (charged-only) in 50 < PT < 65 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 thrust (charged-only) in 65 < PT < 88 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 thrust (charged-only) in 120 < PT < 150 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 thrust (charged-only) in 150 < PT < 186 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 thrust (charged-only) in 186 < PT < 254 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 thrust (charged-only) in 254 < PT < 326 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 thrust (charged-only) in 326 < PT < 408 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 thrust (charged-only) in 408 < PT < 481 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 thrust (charged-only) in 481 < PT < 614 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 thrust (charged-only) in 614 < PT < 800 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 thrust (charged-only) in 800 < PT < 1000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 thrust (charged-only) in 1000 < PT < 4000 GeV in the central dijet region.
Particle-level distributions of groomed AK4 thrust (charged-only) in 50 < PT < 65 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 thrust (charged-only) in 65 < PT < 88 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 thrust (charged-only) in 88 < PT < 120 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 thrust (charged-only) in 120 < PT < 150 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 thrust (charged-only) in 150 < PT < 186 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 thrust (charged-only) in 186 < PT < 254 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 thrust (charged-only) in 254 < PT < 326 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 thrust (charged-only) in 326 < PT < 408 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 thrust (charged-only) in 408 < PT < 481 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 thrust (charged-only) in 481 < PT < 614 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 thrust (charged-only) in 614 < PT < 800 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 thrust (charged-only) in 800 < PT < 1000 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 width (charged-only) in 50 < PT < 65 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 width (charged-only) in 65 < PT < 88 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 width (charged-only) in 88 < PT < 120 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 width (charged-only) in 120 < PT < 150 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 width (charged-only) in 150 < PT < 186 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 width (charged-only) in 186 < PT < 254 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 width (charged-only) in 254 < PT < 326 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 width (charged-only) in 326 < PT < 408 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 width (charged-only) in 408 < PT < 1500 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 width (charged-only) in 50 < PT < 65 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 width (charged-only) in 65 < PT < 88 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 width (charged-only) in 88 < PT < 120 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 width (charged-only) in 120 < PT < 150 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 width (charged-only) in 150 < PT < 186 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 width (charged-only) in 186 < PT < 254 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 width (charged-only) in 254 < PT < 326 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 width (charged-only) in 326 < PT < 408 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 width (charged-only) in 408 < PT < 1500 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 width (charged-only) in 50 < PT < 65 GeV in the central dijet region.
Particle-level distributions of groomed AK4 width (charged-only) in 65 < PT < 88 GeV in the central dijet region.
Particle-level distributions of groomed AK4 width (charged-only) in 88 < PT < 120 GeV in the central dijet region.
Particle-level distributions of groomed AK4 width (charged-only) in 120 < PT < 150 GeV in the central dijet region.
Particle-level distributions of groomed AK4 width (charged-only) in 150 < PT < 186 GeV in the central dijet region.
Particle-level distributions of groomed AK4 width (charged-only) in 186 < PT < 254 GeV in the central dijet region.
Particle-level distributions of groomed AK4 width (charged-only) in 254 < PT < 326 GeV in the central dijet region.
Particle-level distributions of groomed AK4 width (charged-only) in 326 < PT < 408 GeV in the central dijet region.
Particle-level distributions of groomed AK4 width (charged-only) in 408 < PT < 481 GeV in the central dijet region.
Particle-level distributions of groomed AK4 width (charged-only) in 481 < PT < 614 GeV in the central dijet region.
Particle-level distributions of groomed AK4 width (charged-only) in 614 < PT < 800 GeV in the central dijet region.
Particle-level distributions of groomed AK4 width (charged-only) in 800 < PT < 1000 GeV in the central dijet region.
Particle-level distributions of groomed AK4 width (charged-only) in 1000 < PT < 4000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 width (charged-only) in 65 < PT < 88 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 width (charged-only) in 88 < PT < 120 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 width (charged-only) in 120 < PT < 150 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 width (charged-only) in 150 < PT < 186 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 width (charged-only) in 186 < PT < 254 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 width (charged-only) in 254 < PT < 326 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 width (charged-only) in 408 < PT < 481 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 width (charged-only) in 481 < PT < 614 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 width (charged-only) in 614 < PT < 800 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 width (charged-only) in 800 < PT < 1000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 width (charged-only) in 1000 < PT < 4000 GeV in the central dijet region.
Particle-level distributions of groomed AK4 width (charged-only) in 50 < PT < 65 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 width (charged-only) in 65 < PT < 88 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 width (charged-only) in 88 < PT < 120 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 width (charged-only) in 120 < PT < 150 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 width (charged-only) in 150 < PT < 186 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 width (charged-only) in 186 < PT < 254 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 width (charged-only) in 254 < PT < 326 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 width (charged-only) in 326 < PT < 408 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 width (charged-only) in 408 < PT < 481 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 width (charged-only) in 481 < PT < 614 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 width (charged-only) in 800 < PT < 1000 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 width (charged-only) in 1000 < PT < 4000 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 multiplicity in 50 < PT < 65 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 multiplicity in 65 < PT < 88 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 multiplicity in 88 < PT < 120 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 multiplicity in 120 < PT < 150 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 multiplicity in 150 < PT < 186 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 multiplicity in 186 < PT < 254 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 multiplicity in 254 < PT < 326 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 multiplicity in 326 < PT < 408 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 multiplicity in 408 < PT < 1500 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity in 50 < PT < 65 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity in 65 < PT < 88 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity in 88 < PT < 120 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity in 120 < PT < 150 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity in 150 < PT < 186 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity in 186 < PT < 254 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity in 254 < PT < 326 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity in 326 < PT < 408 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity in 408 < PT < 1500 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 multiplicity in 65 < PT < 88 GeV in the central dijet region.
Particle-level distributions of groomed AK4 multiplicity in 88 < PT < 120 GeV in the central dijet region.
Particle-level distributions of groomed AK4 multiplicity in 120 < PT < 150 GeV in the central dijet region.
Particle-level distributions of groomed AK4 multiplicity in 150 < PT < 186 GeV in the central dijet region.
Particle-level distributions of groomed AK4 multiplicity in 186 < PT < 254 GeV in the central dijet region.
Particle-level distributions of groomed AK4 multiplicity in 254 < PT < 326 GeV in the central dijet region.
Particle-level distributions of groomed AK4 multiplicity in 326 < PT < 408 GeV in the central dijet region.
Particle-level distributions of groomed AK4 multiplicity in 408 < PT < 481 GeV in the central dijet region.
Particle-level distributions of groomed AK4 multiplicity in 481 < PT < 614 GeV in the central dijet region.
Particle-level distributions of groomed AK4 multiplicity in 614 < PT < 800 GeV in the central dijet region.
Particle-level distributions of groomed AK4 multiplicity in 800 < PT < 1000 GeV in the central dijet region.
Particle-level distributions of groomed AK4 multiplicity in 1000 < PT < 4000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity in 50 < PT < 65 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity in 65 < PT < 88 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity in 88 < PT < 120 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity in 120 < PT < 150 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity in 150 < PT < 186 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity in 186 < PT < 254 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity in 254 < PT < 326 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity in 326 < PT < 408 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity in 408 < PT < 481 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity in 481 < PT < 614 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity in 614 < PT < 800 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity in 800 < PT < 1000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity in 1000 < PT < 4000 GeV in the central dijet region.
Particle-level distributions of groomed AK4 multiplicity in 50 < PT < 65 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 multiplicity in 65 < PT < 88 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 multiplicity in 88 < PT < 120 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 multiplicity in 120 < PT < 150 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 multiplicity in 150 < PT < 186 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 multiplicity in 186 < PT < 254 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 multiplicity in 254 < PT < 326 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 multiplicity in 326 < PT < 408 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 multiplicity in 481 < PT < 614 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 multiplicity in 614 < PT < 800 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 multiplicity in 800 < PT < 1000 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 multiplicity in 1000 < PT < 4000 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 pTD2 in 50 < PT < 65 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 pTD2 in 65 < PT < 88 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 pTD2 in 88 < PT < 120 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 pTD2 in 120 < PT < 150 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 pTD2 in 150 < PT < 186 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 pTD2 in 186 < PT < 254 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 pTD2 in 254 < PT < 326 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 pTD2 in 326 < PT < 408 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 pTD2 in 408 < PT < 1500 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 in 50 < PT < 65 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 in 65 < PT < 88 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 in 88 < PT < 120 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 in 120 < PT < 150 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 in 150 < PT < 186 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 in 186 < PT < 254 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 in 254 < PT < 326 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 in 326 < PT < 408 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 in 408 < PT < 1500 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 pTD2 in 50 < PT < 65 GeV in the central dijet region.
Particle-level distributions of groomed AK4 pTD2 in 65 < PT < 88 GeV in the central dijet region.
Particle-level distributions of groomed AK4 pTD2 in 88 < PT < 120 GeV in the central dijet region.
Particle-level distributions of groomed AK4 pTD2 in 120 < PT < 150 GeV in the central dijet region.
Particle-level distributions of groomed AK4 pTD2 in 150 < PT < 186 GeV in the central dijet region.
Particle-level distributions of groomed AK4 pTD2 in 186 < PT < 254 GeV in the central dijet region.
Particle-level distributions of groomed AK4 pTD2 in 254 < PT < 326 GeV in the central dijet region.
Particle-level distributions of groomed AK4 pTD2 in 408 < PT < 481 GeV in the central dijet region.
Particle-level distributions of groomed AK4 pTD2 in 481 < PT < 614 GeV in the central dijet region.
Particle-level distributions of groomed AK4 pTD2 in 614 < PT < 800 GeV in the central dijet region.
Particle-level distributions of groomed AK4 pTD2 in 800 < PT < 1000 GeV in the central dijet region.
Particle-level distributions of groomed AK4 pTD2 in 1000 < PT < 4000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 in 50 < PT < 65 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 in 65 < PT < 88 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 in 88 < PT < 120 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 in 120 < PT < 150 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 in 150 < PT < 186 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 in 186 < PT < 254 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 in 254 < PT < 326 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 in 326 < PT < 408 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 in 408 < PT < 481 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 in 481 < PT < 614 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 in 614 < PT < 800 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 in 800 < PT < 1000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 in 1000 < PT < 4000 GeV in the central dijet region.
Particle-level distributions of groomed AK4 pTD2 in 50 < PT < 65 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 pTD2 in 65 < PT < 88 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 pTD2 in 88 < PT < 120 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 pTD2 in 120 < PT < 150 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 pTD2 in 150 < PT < 186 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 pTD2 in 186 < PT < 254 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 pTD2 in 254 < PT < 326 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 pTD2 in 326 < PT < 408 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 pTD2 in 408 < PT < 481 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 pTD2 in 481 < PT < 614 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 pTD2 in 800 < PT < 1000 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 pTD2 in 1000 < PT < 4000 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 thrust in 50 < PT < 65 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 thrust in 65 < PT < 88 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 thrust in 88 < PT < 120 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 thrust in 120 < PT < 150 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 thrust in 150 < PT < 186 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 thrust in 186 < PT < 254 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 thrust in 254 < PT < 326 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 thrust in 326 < PT < 408 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 thrust in 408 < PT < 1500 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 thrust in 50 < PT < 65 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 thrust in 65 < PT < 88 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 thrust in 88 < PT < 120 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 thrust in 120 < PT < 150 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 thrust in 150 < PT < 186 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 thrust in 186 < PT < 254 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 thrust in 254 < PT < 326 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 thrust in 326 < PT < 408 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 thrust in 408 < PT < 1500 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 thrust in 50 < PT < 65 GeV in the central dijet region.
Particle-level distributions of groomed AK4 thrust in 65 < PT < 88 GeV in the central dijet region.
Particle-level distributions of groomed AK4 thrust in 88 < PT < 120 GeV in the central dijet region.
Particle-level distributions of groomed AK4 thrust in 120 < PT < 150 GeV in the central dijet region.
Particle-level distributions of groomed AK4 thrust in 150 < PT < 186 GeV in the central dijet region.
Particle-level distributions of groomed AK4 thrust in 186 < PT < 254 GeV in the central dijet region.
Particle-level distributions of groomed AK4 thrust in 254 < PT < 326 GeV in the central dijet region.
Particle-level distributions of groomed AK4 thrust in 326 < PT < 408 GeV in the central dijet region.
Particle-level distributions of groomed AK4 thrust in 408 < PT < 481 GeV in the central dijet region.
Particle-level distributions of groomed AK4 thrust in 481 < PT < 614 GeV in the central dijet region.
Particle-level distributions of groomed AK4 thrust in 614 < PT < 800 GeV in the central dijet region.
Particle-level distributions of groomed AK4 thrust in 800 < PT < 1000 GeV in the central dijet region.
Particle-level distributions of groomed AK4 thrust in 1000 < PT < 4000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 thrust in 50 < PT < 65 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 thrust in 65 < PT < 88 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 thrust in 88 < PT < 120 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 thrust in 120 < PT < 150 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 thrust in 150 < PT < 186 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 thrust in 186 < PT < 254 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 thrust in 254 < PT < 326 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 thrust in 326 < PT < 408 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 thrust in 408 < PT < 481 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 thrust in 481 < PT < 614 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 thrust in 614 < PT < 800 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 thrust in 800 < PT < 1000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 thrust in 1000 < PT < 4000 GeV in the central dijet region.
Particle-level distributions of groomed AK4 thrust in 50 < PT < 65 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 thrust in 65 < PT < 88 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 thrust in 88 < PT < 120 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 thrust in 120 < PT < 150 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 thrust in 150 < PT < 186 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 thrust in 186 < PT < 254 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 thrust in 326 < PT < 408 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 thrust in 408 < PT < 481 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 thrust in 481 < PT < 614 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 thrust in 614 < PT < 800 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 thrust in 800 < PT < 1000 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 thrust in 1000 < PT < 4000 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 width in 50 < PT < 65 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 width in 65 < PT < 88 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 width in 88 < PT < 120 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 width in 120 < PT < 150 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 width in 150 < PT < 186 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 width in 186 < PT < 254 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 width in 254 < PT < 326 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 width in 326 < PT < 408 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 width in 408 < PT < 1500 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 width in 50 < PT < 65 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 width in 65 < PT < 88 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 width in 88 < PT < 120 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 width in 120 < PT < 150 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 width in 150 < PT < 186 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 width in 186 < PT < 254 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 width in 254 < PT < 326 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 width in 326 < PT < 408 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 width in 408 < PT < 1500 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 width in 50 < PT < 65 GeV in the central dijet region.
Particle-level distributions of groomed AK4 width in 65 < PT < 88 GeV in the central dijet region.
Particle-level distributions of groomed AK4 width in 88 < PT < 120 GeV in the central dijet region.
Particle-level distributions of groomed AK4 width in 120 < PT < 150 GeV in the central dijet region.
Particle-level distributions of groomed AK4 width in 150 < PT < 186 GeV in the central dijet region.
Particle-level distributions of groomed AK4 width in 254 < PT < 326 GeV in the central dijet region.
Particle-level distributions of groomed AK4 width in 326 < PT < 408 GeV in the central dijet region.
Particle-level distributions of groomed AK4 width in 408 < PT < 481 GeV in the central dijet region.
Particle-level distributions of groomed AK4 width in 481 < PT < 614 GeV in the central dijet region.
Particle-level distributions of groomed AK4 width in 614 < PT < 800 GeV in the central dijet region.
Particle-level distributions of groomed AK4 width in 800 < PT < 1000 GeV in the central dijet region.
Particle-level distributions of groomed AK4 width in 1000 < PT < 4000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 width in 50 < PT < 65 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 width in 65 < PT < 88 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 width in 88 < PT < 120 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 width in 120 < PT < 150 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 width in 150 < PT < 186 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 width in 186 < PT < 254 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 width in 254 < PT < 326 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 width in 326 < PT < 408 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 width in 408 < PT < 481 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 width in 481 < PT < 614 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 width in 614 < PT < 800 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 width in 800 < PT < 1000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 width in 1000 < PT < 4000 GeV in the central dijet region.
Particle-level distributions of groomed AK4 width in 50 < PT < 65 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 width in 65 < PT < 88 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 width in 88 < PT < 120 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 width in 120 < PT < 150 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 width in 150 < PT < 186 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 width in 186 < PT < 254 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 width in 254 < PT < 326 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 width in 326 < PT < 408 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 width in 408 < PT < 481 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 width in 614 < PT < 800 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 width in 800 < PT < 1000 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 width in 1000 < PT < 4000 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 LHA in 50 < PT < 65 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 LHA in 65 < PT < 88 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 LHA in 88 < PT < 120 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 LHA in 150 < PT < 186 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 LHA in 186 < PT < 254 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 LHA in 254 < PT < 326 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 LHA in 326 < PT < 408 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 LHA in 408 < PT < 1500 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 LHA in 50 < PT < 65 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 LHA in 65 < PT < 88 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 LHA in 88 < PT < 120 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 LHA in 150 < PT < 186 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 LHA in 186 < PT < 254 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 LHA in 254 < PT < 326 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 LHA in 326 < PT < 408 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 LHA in 408 < PT < 481 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 LHA in 481 < PT < 614 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 LHA in 614 < PT < 800 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 LHA in 800 < PT < 1000 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 LHA in 1000 < PT < 4000 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 LHA in 65 < PT < 88 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 LHA in 88 < PT < 120 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 LHA in 120 < PT < 150 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 LHA in 150 < PT < 186 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 LHA in 186 < PT < 254 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 LHA in 254 < PT < 326 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 LHA in 326 < PT < 408 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 LHA in 408 < PT < 481 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 LHA in 481 < PT < 614 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 LHA in 614 < PT < 800 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 LHA in 1000 < PT < 4000 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 LHA (charged-only) in 50 < PT < 65 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 LHA (charged-only) in 65 < PT < 88 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 LHA (charged-only) in 120 < PT < 150 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 LHA (charged-only) in 150 < PT < 186 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 LHA (charged-only) in 186 < PT < 254 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 LHA (charged-only) in 326 < PT < 408 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 LHA (charged-only) in 408 < PT < 1500 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 LHA (charged-only) in 50 < PT < 65 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 LHA (charged-only) in 65 < PT < 88 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 LHA (charged-only) in 88 < PT < 120 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 LHA (charged-only) in 120 < PT < 150 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 LHA (charged-only) in 150 < PT < 186 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 LHA (charged-only) in 186 < PT < 254 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 LHA (charged-only) in 254 < PT < 326 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 LHA (charged-only) in 326 < PT < 408 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 LHA (charged-only) in 408 < PT < 1500 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 LHA (charged-only) in 50 < PT < 65 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 LHA (charged-only) in 88 < PT < 120 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 LHA (charged-only) in 120 < PT < 150 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 LHA (charged-only) in 150 < PT < 186 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 LHA (charged-only) in 186 < PT < 254 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 LHA (charged-only) in 254 < PT < 326 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 LHA (charged-only) in 326 < PT < 408 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 LHA (charged-only) in 408 < PT < 481 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 LHA (charged-only) in 481 < PT < 614 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 LHA (charged-only) in 614 < PT < 800 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 LHA (charged-only) in 800 < PT < 1000 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 LHA (charged-only) in 1000 < PT < 4000 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 LHA (charged-only) in 50 < PT < 65 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 LHA (charged-only) in 65 < PT < 88 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 LHA (charged-only) in 88 < PT < 120 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 LHA (charged-only) in 120 < PT < 150 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 LHA (charged-only) in 150 < PT < 186 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 LHA (charged-only) in 186 < PT < 254 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 LHA (charged-only) in 254 < PT < 326 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 LHA (charged-only) in 326 < PT < 408 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 LHA (charged-only) in 408 < PT < 481 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 LHA (charged-only) in 481 < PT < 614 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 LHA (charged-only) in 614 < PT < 800 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 LHA (charged-only) in 800 < PT < 1000 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 LHA (charged-only) in 1000 < PT < 4000 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 multiplicity (charged-only) in 50 < PT < 65 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 multiplicity (charged-only) in 65 < PT < 88 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 multiplicity (charged-only) in 88 < PT < 120 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 multiplicity (charged-only) in 120 < PT < 150 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 multiplicity (charged-only) in 150 < PT < 186 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 multiplicity (charged-only) in 186 < PT < 254 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 multiplicity (charged-only) in 254 < PT < 326 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 multiplicity (charged-only) in 326 < PT < 408 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 multiplicity (charged-only) in 50 < PT < 65 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 multiplicity (charged-only) in 65 < PT < 88 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 multiplicity (charged-only) in 88 < PT < 120 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 multiplicity (charged-only) in 120 < PT < 150 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 multiplicity (charged-only) in 150 < PT < 186 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 multiplicity (charged-only) in 186 < PT < 254 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 multiplicity (charged-only) in 254 < PT < 326 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 multiplicity (charged-only) in 326 < PT < 408 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 multiplicity (charged-only) in 408 < PT < 1500 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 multiplicity (charged-only) in 50 < PT < 65 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 multiplicity (charged-only) in 65 < PT < 88 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 multiplicity (charged-only) in 120 < PT < 150 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 multiplicity (charged-only) in 150 < PT < 186 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 multiplicity (charged-only) in 186 < PT < 254 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 multiplicity (charged-only) in 254 < PT < 326 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 multiplicity (charged-only) in 326 < PT < 408 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 multiplicity (charged-only) in 408 < PT < 481 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 multiplicity (charged-only) in 481 < PT < 614 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 multiplicity (charged-only) in 614 < PT < 800 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 multiplicity (charged-only) in 800 < PT < 1000 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 multiplicity (charged-only) in 1000 < PT < 4000 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 multiplicity (charged-only) in 50 < PT < 65 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 multiplicity (charged-only) in 65 < PT < 88 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 multiplicity (charged-only) in 88 < PT < 120 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 multiplicity (charged-only) in 120 < PT < 150 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 multiplicity (charged-only) in 150 < PT < 186 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 multiplicity (charged-only) in 186 < PT < 254 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 multiplicity (charged-only) in 254 < PT < 326 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 multiplicity (charged-only) in 326 < PT < 408 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 multiplicity (charged-only) in 408 < PT < 481 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 multiplicity (charged-only) in 481 < PT < 614 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 multiplicity (charged-only) in 614 < PT < 800 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 multiplicity (charged-only) in 800 < PT < 1000 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 multiplicity (charged-only) in 1000 < PT < 4000 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 pTD2 (charged-only) in 50 < PT < 65 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 pTD2 (charged-only) in 65 < PT < 88 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 pTD2 (charged-only) in 88 < PT < 120 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 pTD2 (charged-only) in 120 < PT < 150 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 pTD2 (charged-only) in 150 < PT < 186 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 pTD2 (charged-only) in 186 < PT < 254 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 pTD2 (charged-only) in 326 < PT < 408 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 pTD2 (charged-only) in 408 < PT < 1500 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 pTD2 (charged-only) in 50 < PT < 65 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 pTD2 (charged-only) in 65 < PT < 88 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 pTD2 (charged-only) in 88 < PT < 120 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 pTD2 (charged-only) in 120 < PT < 150 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 pTD2 (charged-only) in 150 < PT < 186 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 pTD2 (charged-only) in 186 < PT < 254 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 pTD2 (charged-only) in 254 < PT < 326 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 pTD2 (charged-only) in 326 < PT < 408 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 pTD2 (charged-only) in 408 < PT < 1500 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 pTD2 (charged-only) in 50 < PT < 65 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 pTD2 (charged-only) in 65 < PT < 88 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 pTD2 (charged-only) in 88 < PT < 120 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 pTD2 (charged-only) in 120 < PT < 150 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 pTD2 (charged-only) in 150 < PT < 186 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 pTD2 (charged-only) in 186 < PT < 254 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 pTD2 (charged-only) in 254 < PT < 326 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 pTD2 (charged-only) in 326 < PT < 408 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 pTD2 (charged-only) in 408 < PT < 481 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 pTD2 (charged-only) in 481 < PT < 614 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 pTD2 (charged-only) in 614 < PT < 800 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 pTD2 (charged-only) in 800 < PT < 1000 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 pTD2 (charged-only) in 1000 < PT < 4000 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 pTD2 (charged-only) in 50 < PT < 65 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 pTD2 (charged-only) in 65 < PT < 88 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 pTD2 (charged-only) in 88 < PT < 120 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 pTD2 (charged-only) in 120 < PT < 150 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 pTD2 (charged-only) in 186 < PT < 254 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 pTD2 (charged-only) in 254 < PT < 326 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 pTD2 (charged-only) in 326 < PT < 408 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 pTD2 (charged-only) in 408 < PT < 481 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 pTD2 (charged-only) in 481 < PT < 614 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 pTD2 (charged-only) in 614 < PT < 800 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 pTD2 (charged-only) in 800 < PT < 1000 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 pTD2 (charged-only) in 1000 < PT < 4000 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 thrust (charged-only) in 50 < PT < 65 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 thrust (charged-only) in 65 < PT < 88 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 thrust (charged-only) in 88 < PT < 120 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 thrust (charged-only) in 120 < PT < 150 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 thrust (charged-only) in 150 < PT < 186 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 thrust (charged-only) in 186 < PT < 254 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 thrust (charged-only) in 254 < PT < 326 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 thrust (charged-only) in 326 < PT < 408 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 thrust (charged-only) in 408 < PT < 1500 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 thrust (charged-only) in 50 < PT < 65 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 thrust (charged-only) in 65 < PT < 88 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 thrust (charged-only) in 88 < PT < 120 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 thrust (charged-only) in 120 < PT < 150 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 thrust (charged-only) in 150 < PT < 186 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 thrust (charged-only) in 186 < PT < 254 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 thrust (charged-only) in 254 < PT < 326 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 thrust (charged-only) in 326 < PT < 408 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 thrust (charged-only) in 408 < PT < 1500 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 thrust (charged-only) in 50 < PT < 65 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 thrust (charged-only) in 65 < PT < 88 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 thrust (charged-only) in 88 < PT < 120 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 thrust (charged-only) in 150 < PT < 186 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 thrust (charged-only) in 186 < PT < 254 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 thrust (charged-only) in 254 < PT < 326 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 thrust (charged-only) in 326 < PT < 408 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 thrust (charged-only) in 408 < PT < 481 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 thrust (charged-only) in 481 < PT < 614 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 thrust (charged-only) in 614 < PT < 800 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 thrust (charged-only) in 800 < PT < 1000 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 thrust (charged-only) in 1000 < PT < 4000 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 thrust (charged-only) in 50 < PT < 65 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 thrust (charged-only) in 65 < PT < 88 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 thrust (charged-only) in 88 < PT < 120 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 thrust (charged-only) in 120 < PT < 150 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 thrust (charged-only) in 150 < PT < 186 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 thrust (charged-only) in 186 < PT < 254 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 thrust (charged-only) in 254 < PT < 326 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 thrust (charged-only) in 326 < PT < 408 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 thrust (charged-only) in 408 < PT < 481 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 thrust (charged-only) in 481 < PT < 614 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 thrust (charged-only) in 614 < PT < 800 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 thrust (charged-only) in 800 < PT < 1000 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 thrust (charged-only) in 1000 < PT < 4000 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK8 width (charged-only) in 50 < PT < 65 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 width (charged-only) in 65 < PT < 88 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 width (charged-only) in 88 < PT < 120 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 width (charged-only) in 150 < PT < 186 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 width (charged-only) in 186 < PT < 254 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 width (charged-only) in 254 < PT < 326 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 width (charged-only) in 326 < PT < 408 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 width (charged-only) in 408 < PT < 1500 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 width (charged-only) in 50 < PT < 65 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 width (charged-only) in 65 < PT < 88 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 width (charged-only) in 88 < PT < 120 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 width (charged-only) in 120 < PT < 150 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 width (charged-only) in 150 < PT < 186 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 width (charged-only) in 186 < PT < 254 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 width (charged-only) in 254 < PT < 326 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 width (charged-only) in 326 < PT < 408 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK8 width (charged-only) in 408 < PT < 1500 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK8 width (charged-only) in 50 < PT < 65 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 width (charged-only) in 65 < PT < 88 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 width (charged-only) in 88 < PT < 120 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 width (charged-only) in 120 < PT < 150 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 width (charged-only) in 150 < PT < 186 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 width (charged-only) in 186 < PT < 254 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 width (charged-only) in 254 < PT < 326 GeV in the central dijet region.
Particle-level distributions of ungroomed AK8 width (charged-only) in 326 < PT < 408 GeV in the central dijet region.
A measurement of inclusive four-jet production in proton-proton collisions at a center-of-mass energy of 13\TeV is presented. The transverse momenta of jets within $\lvert\eta\rvert \lt$ 4.7 reach down to 35, 30, 25, and 20 GeV for the first-, second-, third-, and fourth-leading jet, respectively. Differential cross sections are measured as functions of the jet transverse momentum, jet pseudorapidity, and several other observables that describe the angular correlations between the jets. The measured distributions show sensitivity to different aspects of the underlying event, parton shower, and matrix element calculations. In particular, the interplay between angular correlations caused by parton shower and double-parton scattering contributions is shown to be important. The double-parton scattering contribution is extracted by means of a template fit to the data, using distributions for single-parton scattering obtained from Monte Carlo event generators and a double-parton scattering distribution constructed from inclusive single-jet events in data. The effective double-parton scattering cross section is calculated and discussed in view of previous measurements and of its dependence on the models used to describe the single-parton scattering background.
Comparison of the pT spectrum for the leading jet from data to different PYTHIA8 (P8),HERWIG++ (H++),and HERWIG7 (H7) tunes.
Comparison of the pT spectrum for the sub-leading from data to different PYTHIA8 (P8),HERWIG++ (H++),and HERWIG7 (H7) tunes.
Comparison of the pT spectrum for the third-leading from data to different PYTHIA8 (P8),HERWIG++ (H++),and HERWIG7 (H7) tunes.
Comparison of the pT spectrum for the fourth-leading from data to different PYTHIA8 (P8),HERWIG++ (H++),and HERWIG7 (H7) tunes.
Comparison of the eta spectrum for the leading jet from data to different PYTHIA8 (P8),HERWIG++ (H++),and HERWIG7 (H7) tunes.
Comparison of the eta spectrum for the sub-leading from data to different PYTHIA8 (P8),HERWIG++ (H++),and HERWIG7 (H7) tunes.
Comparison of the eta spectrum for the third-leading from data to different PYTHIA8 (P8),HERWIG++ (H++),and HERWIG7 (H7) tunes.
Comparison of the eta spectrum for the fourth-leading from data to different PYTHIA8 (P8),HERWIG++ (H++),and HERWIG7 (H7) tunes.
Comparison of the DeltaPhiSoft distribution from data to different PYTHIA8 (P8),HERWIG++ (H++), and HERWIG7 (H7) tunes. All distributions have been normalized to regions where a reduced DPS contribution is expected.
Comparison of the DeltaPhiMin distribution from data to different PYTHIA8 (P8),HERWIG++ (H++), and HERWIG7 (H7) tunes. All distributions have been normalized to regions where a reduced DPS contribution is expected.
Comparison of the DeltaY distribution from data to different PYTHIA8 (P8),HERWIG++ (H++), and HERWIG7 (H7) tunes. All distributions have been normalized to regions where a reduced DPS contribution is expected.
Comparison of the phi_ij distribution from data to different PYTHIA8 (P8),HERWIG++ (H++), and HERWIG7 (H7) tunes. All distributions have been normalized to regions where a reduced DPS contribution is expected.
Comparison of the Deltap_{T,Soft} distribution from data to different PYTHIA 8 (P8), HERWIG ++ (H++), and HERWIG 7 (H7) tunes. All distributions have been normalized to regions where a reduced DPS contribution is expected.
Comparison of the DeltaS distribution from data to different PYTHIA 8 (P8), HERWIG ++ (H++), and HERWIG 7 (H7) tunes. All distributions have been normalized to regions where a reduced DPS contribution is expected.
Comparison of the pT spectrum for the leading jet from data with different KATIE(KT), MADGRAPH5aMC@NLO(MG5), and POWHEG(PW) models
Comparison of the pT spectrum for the sub-leading from data with different KATIE(KT), MADGRAPH5aMC@NLO(MG5), and POWHEG(PW) models
Comparison of the pT spectrum for the third-leading from data to different PYTHIA8 (P8),HERWIG++ (H++),and HERWIG7 (H7) tunes.
Comparison of the pT spectrum for the fourth-leading from data with different KATIE(KT), MADGRAPH5aMC@NLO(MG5), and POWHEG(PW) models
Comparison of the eta spectrum for the leading jet from data with different KATIE(KT), MADGRAPH5aMC@NLO(MG5), and POWHEG(PW) models
Comparison of the eta spectrum for the sub-leading from data with different KATIE(KT), MADGRAPH5aMC@NLO(MG5), and POWHEG(PW) models
Comparison of the eta spectrum for the third-leading from data with different KATIE(KT), MADGRAPH5aMC@NLO(MG5), and POWHEG(PW) models
Comparison of the eta spectrum for the fourth-leading from data with different KATIE(KT), MADGRAPH5aMC@NLO(MG5), and POWHEG(PW) models
Comparison of the DeltaPhiSoft distribution from data to differentKATIE(KT), MADGRAPH5aMC@NLO(MG5), andPOWHEG(PW) implementations. All distributions have been normalized to regions where a reduced DPS sensitivity is expected.
Comparison of the DeltaPhiMin, distribution from data to differentKATIE(KT), MADGRAPH5aMC@NLO(MG5), andPOWHEG(PW) implementations. All distributions have been normalized to regions where a reduced DPS sensitivity is expected.
Comparison of the DeltaY and distribution from data to differentKATIE(KT), MADGRAPH5aMC@NLO(MG5), andPOWHEG(PW) implementations. All distributions have been normalized to regions where a reduced DPS sensitivity is expected.
Comparison of the phi_ij distribution from data to differentKATIE(KT), MADGRAPH5aMC@NLO(MG5), andPOWHEG(PW) implementations. All distributions have been normalized to regions where a reduced DPS sensitivity is expected.
Comparison of the Deltap_{T,Soft} distribution from data to different KATIE(KT),MADGRAPH5aMC@NLO(MG5), andPOWHEG(PW) implementations. All distributions havebeen normalized to regions where a reduced DPS sensitivity is expected.
Comparison of the DeltaS distribution from data to different KATIE(KT),MADGRAPH5aMC@NLO(MG5), andPOWHEG(PW) implementations. All distributions havebeen normalized to regions where a reduced DPS sensitivity is expected.
Comparison of the pT spectrum for the leading jet from data with different SPS+DPS KATIE( KT) and PYTHIA8 (P8) models.
Comparison of the pT spectrum for the sub-leading from data with different SPS+DPS KATIE( KT) and PYTHIA8 (P8) models.
Comparison of the pT spectrum for the third-leading from data with different SPS+DPS KATIE( KT) and PYTHIA8 (P8) models.
Comparison of the pT spectrum for the fourth-leading from data with different SPS+DPS KATIE( KT) and PYTHIA8 (P8) models.
Comparison of the eta spectrum for the leading jet from data with different SPS+DPS KATIE( KT) and PYTHIA8 (P8) models.
Comparison of the eta spectrum for the sub-leading from data with different SPS+DPS KATIE( KT) and PYTHIA8 (P8) models.
Comparison of the eta spectrum for the third-leading from data with different SPS+DPS KATIE( KT) and PYTHIA8 (P8) models.
Comparison of the eta spectrum for the fourth-leading from data with different SPS+DPS KATIE( KT) and PYTHIA8 (P8) models.
Comparison of the DeltaPhiSoft distribution from data to different SPS+DPS KATIE (KT) and PYTHIA 8 (P8) models. All distributions have been normalized to regions where a reduced DPS sensitivity is expected.
Comparison of the DeltaPhiMin distribution from data to different SPS+DPS KATIE (KT) and PYTHIA 8 (P8) models. All distributions have been normalized to regions where a reduced DPS sensitivity is expected.
Comparison of the DeltaY distribution from data to different SPS+DPS KATIE (KT) and PYTHIA 8 (P8) models. All distributions have been normalized to regions where a reduced DPS sensitivity is expected.
Comparison of the phi_ij distribution from data to different SPS+DPS KATIE (KT) and PYTHIA 8 (P8) models. All distributions have been normalized to regions where a reduced DPS sensitivity is expected.
Comparison of the Deltap_{T,Soft} distributions from data to different SPS+DPS KATIE (KT) and PYTHIA 8 (P8) models. All distributions havebeen normalized to regions where a reduced DPS sensitivity is expected.
Comparison of the DeltaS distributions from data to different SPS+DPS KATIE (KT) and PYTHIA 8 (P8) models. All distributions have been normalized to regions where a reduced DPS contribution is expected.
The DeltaS distribution obtained from the mixed data sample compared to predictions from the pure DPS sample in PYTHIA 8 (P8) and KATIE (KT). The distributions are normalized to unity.
The results of the template fit for the POWHEG (PW) NLO 2 -> 2 model without the hard MPI removed. As the DeltaS distribution obtained from the mixed data sample carries a statistical and systematic uncertainty, so does the total fitted sample.
Comparison of the DeltaPhiSoft distribution from data to different PYTHIA8 (P8),HERWIG++ (H++), and HERWIG7 (H7) tunes.
Comparison of the DeltaPhiMin distribution from data to different PYTHIA8 (P8),HERWIG++ (H++), and HERWIG7 (H7) tunes.
Comparison of the DeltaY distribution from data to different PYTHIA8 (P8),HERWIG++ (H++), and HERWIG7 (H7) tunes.
Comparison of the phi_ij distribution from data to different PYTHIA8 (P8),HERWIG++ (H++), and HERWIG7 (H7) tunes.
Comparison of the Deltap_{T,Soft} distribution from data to different PYTHIA 8 (P8), HERWIG ++ (H++), and HERWIG 7 (H7) tunes.
Comparison of the DeltaS distribution from data to different PYTHIA 8 (P8), HERWIG ++ (H++), and HERWIG 7 (H7) tunes.
Comparison of the DeltaPhiSoft distribution from data to different KATIE(KT),MADGRAPH5aMC@NLO(MG5), andPOWHEG(PW) implementations.
Comparison of the DeltaPhiMin distribution from data to different KATIE(KT),MADGRAPH5aMC@NLO(MG5), andPOWHEG(PW) implementations.
Comparison of the DeltaY distribution from data to different KATIE(KT),MADGRAPH5aMC@NLO(MG5), andPOWHEG(PW) implementations.
Comparison of the phi_ij distribution from data to different KATIE(KT),MADGRAPH5aMC@NLO(MG5), andPOWHEG(PW) implementations.
Comparison of the Deltap_{T,Soft} distribution from data to different KATIE(KT),MADGRAPH5aMC@NLO(MG5), andPOWHEG(PW) implementations.
Comparison of the DeltaS distribution from data to different KATIE(KT),MADGRAPH5aMC@NLO(MG5), andPOWHEG(PW) implementations.
Comparison of the DeltaPhiSoft distribution from data to different SPS+DPS KATIE (KT) and PYTHIA 8 (P8) models.
Comparison of the DeltaPhiMin distribution from data to different SPS+DPS KATIE (KT) and PYTHIA 8 (P8) models.
Comparison of the DeltaY distribution from data to different SPS+DPS KATIE (KT) and PYTHIA 8 (P8) models.
Comparison of the phi_ij distribution from data to different SPS+DPS KATIE (KT) and PYTHIA 8 (P8) models.
Comparison of the Deltap_{T,Soft} distribution from data to different SPS+DPS KATIE (KT) and PYTHIA 8 (P8) models.
Comparison of the DeltaS distributions from data to different SPS+DPS KATIE (KT) and PYTHIA 8 (P8) models.
The measurement of the cross section for the production of a Z boson, decaying to dielectrons or dimuons, in association with at least one bottom quark jet are performed with proton-proton collision data at $\sqrt{s} =$ 13 TeV. The data sample corresponds to an integrated luminosity of 137 fb$^{-1}$, collected by the CMS experiment at the LHC during 2016-2018. The integrated cross sections for Z + $\ge$ 1 b jet and Z + $\ge$ 2 b jets are reported for the electron, muon, and combined channels. The fiducial cross sections in the combined channel are 6.52 $\pm$ 0.04 (stat) $\pm$ 0.40 (syst) $\pm$ 0.14 (theo) pb for Z + $\ge$ 1 b jet and 0.65 $\pm$ 0.03 (stat) $\pm$ 0.07 (syst) $\pm$ 0.02 (theo) pb for Z + $\ge$ 2 b jets. The differential cross section distributions are measured as functions of various kinematic observables that are useful for precision tests of perturbative quantum chromodynamics predictions. The ratios of integrated and differential cross sections for Z + $\ge$ 2 b jets and Z + $\ge$ 1 b jet processes are also determined. The value of the integrated cross section ratio measured in the combined channel is 0.100 $\pm$ 0.005 (stat) $\pm$ 0.007 (syst) $\pm$ 0.003 (theo). All measurements are compared with predictions from various event generators.
The associated production of a W and a Z boson is studied in final states with multiple leptons produced in proton-proton (pp) collisions at a centre-of-mass energy of 13 TeV using 137 fb$^{-1}$ of data collected with the CMS detector at the LHC. A measurement of the total inclusive production cross section yields $\sigma_{\text{tot}}$(pp $\to$ WZ) = 50.6 $\pm$ 0.8 (stat) $\pm$ 1.5 (syst) $\pm$ 1.1 (lumi) $\pm$ 0.5 (theo) pb. Measurements of the fiducial and differential cross sections for several key observables are also performed in all the final-state lepton flavour and charge compositions with a total of three charged leptons, which can be electrons or muons. All results are compared with theoretical predictions computed up to next-to-next-to-leading order in quantum chromodynamics plus next-to-leading order in electroweak theory and for various sets of parton distribution functions. The results include direct measurements of the charge asymmetry and the W and Z vector boson polarization. The first observation of longitudinally polarized W bosons in WZ production is reported. Anomalous gauge couplings are searched for, leading to new constraints on beyond-the-standard-model contributions to the WZ triple gauge coupling.
Distribution of the three leading leptons flavour in the CR-ZZ with uncertainties evaluated after the inclusive cross section fit
Distribution of the jet multiplicity in the CR-ttZ with uncertainties evaluated after the inclusive cross section fit
Distribution of the three leading leptons flavour in the CR-conv with uncertainties evaluated after the inclusive cross section fit
Distribution of the three leading leptons flavour in the SR-WZ with uncertainties evaluated after the inclusive cross section fit
Efficiency, acceptance, and proportion of events with leptonic tau decays in WZ production
WZ fiducial cross section in the four flavour exclusive and the flavour inclusive channels
WZ total cross section extrapolated from the four flavour exclusive and the flavour inclusive channels
Distribution of the total lepton charge in the SR-WZ with uncertainties evaluated after the inclusive cross section fit
W$^{+}$Z fiducial cross section in the four flavour exclusive and the flavour inclusive channels
W$^{-}$Z fiducial cross section in the four flavour exclusive and the flavour inclusive channels
WZ charge asymmetry ratio measured on each of the four flavour exclusive and the flavour inclusive channels
Distribution of the cosine of the W polarization angle times total lepton charge in the SR-WZ with uncertainties evaluated after the W polarization fit
Distribution of the cosine of the Z polarization angle in the SR-WZ with uncertainties evaluated after the Z polarization fit
Best fits to the W and Z polarization fractions
2D confidence regions at the 68, 95, and 99% CL in the $f_O^W$-$f_{L}^W-f_R^W$ plane
2D confidence regions at the 68, 95, and 99% CL in the $f_O^Z$-$f_{L}^Z-f_R^Z$ plane
Distribution of the invariant mass of the WZ system in the SR-WZ with uncertainties evaluated after the inclusive cross section fit
Best fit values and one dimensional confidence regions in several EFT coefficients obtained from the EFT fit considering both the SM interferences and purely BSM (order $\Lambda^{-2}$ and $\Lambda^{-4}$) terms
2D confidence regions at the 68, 95, and 99% CL in the $c_{www}$-$c_{w}$ plane
2D confidence regions at the 68, 95, and 99% CL in the $c_{w}$-$c_{b}$ plane
2D confidence regions at the 68, 95, and 99% CL in the $c_{www}$-$c_{w}$ plane
Best fit values and one dimensional confidence regions in several EFT coefficients obtained from the EFT fit considering only the SM-EFT interference (order $\Lambda^{-2}$) terms
Evolution of the best fit and expected and observed 95% CI for the $c_{w}$ parameter as a function of the cutoff scale
Evolution of the best fit and expected and observed 95% CI for the $c_{b}$ parameter as a function of the cutoff scale
Evolution of the best fit and expected and observed 95% CI for the $c_{www}$ parameter as a function of the cutoff scale
Evolution of the best fit and expected and observed 95% CI for the $\tilde{c}_{www}$ parameter as a function of the cutoff scale
Evolution of the best fit and expected and observed 95% CI for the $\tilde{c}_{w}$ parameter as a function of the cutoff scale
Differential cross section with respect to the transverse momentum of the Z boson
Correlation matrix for the unfolded results obtained using NNLO bias, area con-straint, and no additional regularization for the $p_{T}$ of the Z boson
Response matrix for the $p_{T}$ of the Z boson obtained with POWHEG
Differential cross section with respect to the transverse momentum of the leading jet
Correlation matrix for the unfolded results obtained using NNLO bias, area con-straint, and no additional regularization for the $p_{T}$ of the leading jet
Response matrix for the $p_{T}$ of the leading jet obtained with POWHEG
Differential cross section with respect to the jet multiplicity
Correlation matrix for the unfolded results obtained using NNLO bias, area con-straint, and no additional regularization for the jet multiplicity
Response matrix for the jet multiplicity obtained with POWHEG
Differential cross section with respect to the invariant mass of the WZ system
Correlation matrix for the unfolded results obtained using NNLO bias, area con-straint, and no additional regularization for the invariant mass of the WZ system
Response matrix for the invariant mass of the WZ system obtained with POWHEG
Differential cross section with respect to the transverse momentum of the lepton associated to the W boson
Correlation matrix for the unfolded results obtained using NNLO bias, area con-straint, and no additional regularization for the $p_{T}$ of the lepton associated to the W boson
Response matrix for the $p_{T}$ of the lepton associated to the W boson obtained with POWHEG
Differential cross section with respect to the transverse momentum of the lepton associated to the W boson, W$^{+}$Z only
Correlation matrix for the unfolded results obtained using NNLO bias, area con-straint, and no additional regularization for the $p_{T}$ of the lepton associated to the W boson, W$^{+}$Z only
Differential cross section with respect to the transverse momentum of the lepton associated to the W boson, W$^{-}$Z only
Correlation matrix for the unfolded results obtained using NNLO bias, area con-straint, and no additional regularization for the $p_{T}$ of the lepton associated to the W boson, W$^{-}$Z only
Differential cross section with respect to the cosine of the W polarization angle times total lepton charge
Correlation matrix for the unfolded results obtained using NNLO bias, area con-straint, and no additional regularization for the cosine of the W polarization angle times total lepton charge
Response matrix for the cosine of the W polarization angle times total lepton charge obtained with POWHEG
Differential cross section with respect to the cosine of the W polarization angle times total lepton charge, W$^{+}$Z only
Correlation matrix for the unfolded results obtained using NNLO bias, area con-straint, and no additional regularization for the cosine of the W polarization angle times total lepton charge, W$^{+}$Z only
Differential cross section with respect to the cosine of the W polarization angle times total lepton charge, W$^{-}$Z only
Correlation matrix for the unfolded results obtained using NNLO bias, area con-straint, and no additional regularization for the cosine of the W polarization angle times total lepton charge, W$^{-}$Z only
Differential cross section with respect to the cosine of the Z polarization angle
Correlation matrix for the unfolded results obtained using NNLO bias, area con-straint, and no additional regularization for the cosine of the Z polarization angle
Response matrix for the cosine of the Z polarization angle obtained with POWHEG
Differential cross section with respect to the cosine of the Z polarization angle, W$^{+}$Z only
Correlation matrix for the unfolded results obtained using NNLO bias, area con-straint, and no additional regularization for the cosine of the Z polarization angle, W$^{+}$Z only
Differential cross section with respect to the cosine of the Z polarization angle, W$^{-}$Z only
Correlation matrix for the unfolded results obtained using NNLO bias, area con-straint, and no additional regularization for the cosine of the Z polarization angle, W$^{-}$Z only
Inclusive and differential cross sections of single top quark production in association with a Z boson are measured in proton-proton collisions at a center-of-mass energy of 13 TeV with a data sample corresponding to an integrated luminosity of 138 fb$^{-1}$ recorded by the CMS experiment. Events are selected based on the presence of three leptons, electrons or muons, associated with leptonic Z boson and top quark decays. The measurement yields an inclusive cross section of 87.9 $_{-7.3}^{+7.5}$ (stat) $_{-6.0}^{+7.3}$ (syst) fb for a dilepton invariant mass greater than 30 GeV, in agreement with standard model (SM) calculations and the most precise determination to date. The ratio between the cross sections for the top quark and the top antiquark production in association with a Z boson is measured as 2.37 $_{-0.42}^{+0.56}$ (stat) ${}_{-0.13}^{+0.27}$ (syst). Differential measurements at parton and particle levels are performed for the first time. Several kinematic observables are considered to study the modeling of the process. Results are compared to theoretical predictions with different assumptions on the source of the initial-state b quark and found to be in agreement, within the uncertainties. Additionally, the spin asymmetry, which is sensitive to the top quark polarization, is determined from the differential distribution of the polarization angle at parton level to be 0.54 $\pm$ 0.16 (stat) $\pm$ 0.06 (syst), in agreement with SM predictions.
Absolute differential cross sections as a function of the difference in azimuthal angle of the leptons, associated to the Z boson candidate at parton level.
Covariance matrix for the measurement of the differential cross sections as a function of the difference in azimuthal angle of the leptons, associated to the Z boson candidate at parton level.
Covariance matrix for the measurement of the differential cross sections as a function of the difference in azimuthal angle of the leptons, associated to the Z boson candidate at parton level.
Absolute differential cross sections as a function of the difference in azimuthal angle of the leptons, associated to the Z boson candidate at particle level.
Covariance matrix for the measurement of the differential cross sections as a function of the difference in azimuthal angle of the leptons, associated to the Z boson candidate at particle level.
Covariance matrix for the measurement of the differential cross sections as a function of the difference in azimuthal angle of the leptons, associated to the Z boson candidate at particle level.
Normalized differential cross sections as a function of the difference in azimuthal angle of the leptons, associated to the Z boson candidate at parton level.
Normalized differential cross sections as a function of the difference in azimuthal angle of the leptons, associated to the Z boson candidate at particle level.
The production cross section of a top quark pair in association with a photon is measured in proton-proton collisions at a center-of-mass energy of 13 TeV. The data set, corresponding to an integrated luminosity of 137 fb$^{-1}$, was recorded by the CMS experiment during the 2016-2018 data taking of the LHC. The measurements are performed in a fiducial volume defined at the particle level. Events with an isolated, highly energetic lepton, at least three jets from the hadronization of quarks, among which at least one is b tagged, and one isolated photon are selected. The inclusive fiducial $\mathrm{t\overline{t}}\gamma$ cross section, for a photon with transverse momentum greater than 20 GeV and pseudorapidity $\lvert \eta\rvert$$\lt$ 1.4442, is measured to be 798 $\pm$ 7 (stat) $\pm$ 48 (syst) fb, in good agreement with the prediction from the standard model at next-to-leading order in quantum chromodynamics. The differential cross sections are also measured as a function of several kinematic observables and interpreted in the framework of the standard model effective field theory (EFT), leading to the most stringent direct limits to date on anomalous electromagnetic dipole moment interactions of the top quark and the photon.
The production cross section of a top quark pair in association with a photon is measured in proton-proton collisions in the decay channel with two oppositely charged leptons (e$^\pm\mu^\mp$, e$^+$e$^-$, or $\mu^+\mu^-$). The measurement is performed using 138 fb$^{-1}$ of proton-proton collision data recorded by the CMS experiment at $\sqrt{s} =$ 13 TeV during the 2016-2018 data-taking period of the CERN LHC. A fiducial phase space is defined such that photons radiated by initial-state particles, top quarks, or any of their decay products are included. An inclusive cross section of 175.2 $\pm$ 2.5 (stat) $\pm$ 6.3 (syst) fb is measured in a signal region with at least one jet coming from the hadronization of a bottom quark and exactly one photon with transverse momentum above 20 GeV. Differential cross sections are measured as functions of several kinematic observables of the photon, leptons, and jets, and compared to standard model predictions. The measurements are also interpreted in the standard model effective field theory framework, and limits are found on the relevant Wilson coefficients from these results alone and in combination with a previous CMS measurement of the $\mathrm{t\bar{t}}\gamma$ production process using the lepton+jets final state.
A search for heavy neutral leptons (HNLs), the right-handed Dirac or Majorana neutrinos, is performed in final states with three charged leptons (electrons or muons) using proton-proton collision data collected by the CMS experiment at $\sqrt{s} =$ 13 TeV at the CERN LHC. The data correspond to an integrated luminosity of 138 fb$^{-1}$. The HNLs could be produced through mixing with standard model neutrinos $\nu$. For small values of the HNL mass ($\lt$ 20 GeV) and the square of the HNL-$\nu$ mixing parameter (10$^{-7}$-10$^{-2}$), the decay length of these particles can be large enough so that the secondary vertex of the HNL decay can be resolved with the CMS silicon tracker. The selected final state consists of one lepton emerging from the primary proton-proton collision vertex, and two leptons forming a displaced, secondary vertex. No significant deviations from the standard model expectations are observed, and constraints are obtained on the HNL mass and coupling strength parameters, excluding previously unexplored regions of parameter space in the mass range 1-20 GeV and squared mixing parameter values as low as 10$^{-7}$.
Number of predicted and observed events in the $eeX$ final states. The quoted uncertainties include statistical and systematic uncertainties.
Number of predicted and observed events in the $\mu\mu X$ final states. The quoted uncertainties include statistical and systematic uncertainties.
Number of predicted signal events in the $eeX$ final states, for several benchmark signal hypotheses for Majorana HNL. The quoted uncertainties include statistical and systematic uncertainties.
Number of predicted signal events in the $\mu\mu X$ final states, for several benchmark signal hypotheses for Majorana HNL. The quoted uncertainties include statistical and systematic uncertainties.
The 95% CL limits on $|V_{Ne}|^2$ as a function of the HNL mass for a Majorana HNL. Values of $-1$ indicate that no limit is available for the mass point.
The 95% CL limits on $|V_{N\mu}|^2$ as a function of the HNL mass for a Majorana HNL. Values of $-1$ indicate that no limit is available for the mass point.
The 95% CL limits on $|V_{Ne}|^2$ as a function of the HNL mass for a Dirac HNL. Values of $-1$ indicate that no limit is available for the mass point.
The 95% CL limits on $|V_{N\mu}|^2$ as a function of the HNL mass for a Dirac HNL. Values of $-1$ indicate that no limit is available for the mass point.
Mean lifetime and production cross section for HNLs of Majorana nature, assuming the decay to three charged leptons and coupling to only electrons or muons, as evaluated from simulated event samples.
A search is presented for a right-handed W boson (W$_\mathrm{R}$) and a heavy neutrino (N), in a final state consisting of two same-flavor leptons (ee or $\mu\mu$) and two quarks. The search is performed with the CMS experiment at the CERN LHC using a data sample of proton-proton collisions at a center-of-mass energy of 13 TeV corresponding to an integrated luminosity of 138 fb$^{-1}$. The search covers two regions of phase space, one where the decay products of the heavy neutrino are merged into a single large-area jet, and one where the decay products are well separated. The expected signal is characterized by an excess in the invariant mass distribution of the final-state objects. No significant excess over the standard model background expectations is observed. The observations are interpreted as upper limits on the product of W$_\mathrm{R}$ production cross sections and branching fractions assuming that couplings are identical to those of the standard model W boson. For N masses $m_\mathrm{N}$ equal to half the W$_\mathrm{R}$ mass $m_\mathrm{W_R}$ ($m_\mathrm{N}$ = 0.2 TeV), $m_\mathrm{W_R}$ is excluded at 95% confidence level up to 4.7 (4.8) and 5.0 (5.4) TeV for the electron and muon channels, respectively. This analysis provides the most stringent limits on the W$_\mathrm{R}$ mass to date.
Cross sections calculated to next-to-leading (NLO) accuracy
Differential cross section measurements of W$^\pm\gamma$ production in proton-proton collisions at $\sqrt{s}$ = 13 TeV are presented. The data set used in this study was collected with the CMS detector at the CERN LHC in 2016-2018 with an integrated luminosity of 138 fb$^{-1}$. Candidate events containing an electron or muon, a photon, and missing transverse momentum are selected. The measurements are compared with standard model predictions computed at next-to-leading and next-to-next-to-leading orders in perturbative quantum chromodynamics. Constraints on the presence of TeV-scale new physics affecting the WW$\gamma$ vertex are determined within an effective field theory framework, focusing on the $\mathcal{O}_\mathrm{3W}$ operator. A simultaneous measurement of the photon transverse momentum and the azimuthal angle of the charged lepton in a special reference frame is performed. This two-dimensional approach provides up to a factor of ten more sensitivity to the interference between the standard model and the $\mathcal{O}_\mathrm{3W}$ contribution than using the transverse momentum alone.
Measured absolute differential $p_{\mathrm{T}}^{\gamma}$ cross section, compared to the MG5_aMC+PY8, GENEVA, MATRIX and MCFM predictions. The differential cross sections $\sigma_{j}(\mathrm{pp}\rightarrow\mathrm{W}^{\pm}\gamma\rightarrow\ell^{\pm}\nu\gamma)$, where $\ell$ denotes all three lepton flavors, are measured in the following fiducial region: $p_{\mathrm{T}}^{\ell} > 30\,\mathrm{GeV}$, $|\eta^{\ell}| < 2.5$, $p_{\mathrm{T}}^{\gamma} > 30\,\mathrm{GeV}$, $|\eta^{\gamma}| < 2.5$, $p_{\mathrm{T}}^{\mathrm{miss}} > 40\,\mathrm{GeV}$, and $\Delta R(\ell, \gamma) > 0.7$. The leptons are dressed by adding the four-momenta of any photons with $\Delta R(\ell, \gamma) < 0.1$ to the four-momentum of the lepton. A smooth-cone photon isolation is also applied, with parameters $\delta_{0}=0.4$, $\epsilon=1.0$, and $n=1$.
Measured fractional differential $p_{\mathrm{T}}^{\gamma}$ cross section, compared to the MG5_aMC+PY8, GENEVA, MATRIX and MCFM predictions. The differential cross sections $\sigma_{j}(\mathrm{pp}\rightarrow\mathrm{W}^{\pm}\gamma\rightarrow\ell^{\pm}\nu\gamma)$, where $\ell$ denotes all three lepton flavors, are measured in the following fiducial region: $p_{\mathrm{T}}^{\ell} > 30\,\mathrm{GeV}$, $|\eta^{\ell}| < 2.5$, $p_{\mathrm{T}}^{\gamma} > 30\,\mathrm{GeV}$, $|\eta^{\gamma}| < 2.5$, $p_{\mathrm{T}}^{\mathrm{miss}} > 40\,\mathrm{GeV}$, and $\Delta R(\ell, \gamma) > 0.7$. The leptons are dressed by adding the four-momenta of any photons with $\Delta R(\ell, \gamma) < 0.1$ to the four-momentum of the lepton. A smooth-cone photon isolation is also applied, with parameters $\delta_{0}=0.4$, $\epsilon=1.0$, and $n=1$.
Relative uncertainties on the measured absolute differential $p_{\mathrm{T}}^{\gamma}$ cross section.
Relative uncertainties on the measured fractional differential $p_{\mathrm{T}}^{\gamma}$ cross section.
Correlation matrix for the measured absolute differential $p_{\mathrm{T}}^{\gamma}$ cross section.
Correlation matrix for the measured fractional differential $p_{\mathrm{T}}^{\gamma}$ cross section.
Response matrix from the fiducial to the reconstructed bins of the differential $p_{\mathrm{T}}^{\gamma}$ cross section measurement.
Measured absolute differential $\eta^{\gamma}$ cross section, compared to the MG5_aMC+PY8, GENEVA, MATRIX and MCFM predictions. The differential cross sections $\sigma_{j}(\mathrm{pp}\rightarrow\mathrm{W}^{\pm}\gamma\rightarrow\ell^{\pm}\nu\gamma)$, where $\ell$ denotes all three lepton flavors, are measured in the following fiducial region: $p_{\mathrm{T}}^{\ell} > 30\,\mathrm{GeV}$, $|\eta^{\ell}| < 2.5$, $p_{\mathrm{T}}^{\gamma} > 30\,\mathrm{GeV}$, $|\eta^{\gamma}| < 2.5$, $p_{\mathrm{T}}^{\mathrm{miss}} > 40\,\mathrm{GeV}$, and $\Delta R(\ell, \gamma) > 0.7$. The leptons are dressed by adding the four-momenta of any photons with $\Delta R(\ell, \gamma) < 0.1$ to the four-momentum of the lepton. A smooth-cone photon isolation is also applied, with parameters $\delta_{0}=0.4$, $\epsilon=1.0$, and $n=1$.
Measured fractional differential $\eta^{\gamma}$ cross section, compared to the MG5_aMC+PY8, GENEVA, MATRIX and MCFM predictions. The differential cross sections $\sigma_{j}(\mathrm{pp}\rightarrow\mathrm{W}^{\pm}\gamma\rightarrow\ell^{\pm}\nu\gamma)$, where $\ell$ denotes all three lepton flavors, are measured in the following fiducial region: $p_{\mathrm{T}}^{\ell} > 30\,\mathrm{GeV}$, $|\eta^{\ell}| < 2.5$, $p_{\mathrm{T}}^{\gamma} > 30\,\mathrm{GeV}$, $|\eta^{\gamma}| < 2.5$, $p_{\mathrm{T}}^{\mathrm{miss}} > 40\,\mathrm{GeV}$, and $\Delta R(\ell, \gamma) > 0.7$. The leptons are dressed by adding the four-momenta of any photons with $\Delta R(\ell, \gamma) < 0.1$ to the four-momentum of the lepton. A smooth-cone photon isolation is also applied, with parameters $\delta_{0}=0.4$, $\epsilon=1.0$, and $n=1$.
Relative uncertainties on the measured absolute differential $\eta^{\gamma}$ cross section.
Relative uncertainties on the measured fractional differential $\eta^{\gamma}$ cross section.
Correlation matrix for the measured absolute differential $\eta^{\gamma}$ cross section.
Correlation matrix for the measured fractional differential $\eta^{\gamma}$ cross section.
Response matrix from the fiducial to the reconstructed bins of the differential $\eta^{\gamma}$ cross section measurement.
Measured absolute differential $\Delta R(\ell,\gamma)$ cross section, compared to the MG5_aMC+PY8, GENEVA, MATRIX and MCFM predictions. The differential cross sections $\sigma_{j}(\mathrm{pp}\rightarrow\mathrm{W}^{\pm}\gamma\rightarrow\ell^{\pm}\nu\gamma)$, where $\ell$ denotes all three lepton flavors, are measured in the following fiducial region: $p_{\mathrm{T}}^{\ell} > 30\,\mathrm{GeV}$, $|\eta^{\ell}| < 2.5$, $p_{\mathrm{T}}^{\gamma} > 30\,\mathrm{GeV}$, $|\eta^{\gamma}| < 2.5$, $p_{\mathrm{T}}^{\mathrm{miss}} > 40\,\mathrm{GeV}$, and $\Delta R(\ell, \gamma) > 0.7$. The leptons are dressed by adding the four-momenta of any photons with $\Delta R(\ell, \gamma) < 0.1$ to the four-momentum of the lepton. A smooth-cone photon isolation is also applied, with parameters $\delta_{0}=0.4$, $\epsilon=1.0$, and $n=1$.
Measured fractional differential $\Delta R(\ell,\gamma)$ cross section, compared to the MG5_aMC+PY8, GENEVA, MATRIX and MCFM predictions. The differential cross sections $\sigma_{j}(\mathrm{pp}\rightarrow\mathrm{W}^{\pm}\gamma\rightarrow\ell^{\pm}\nu\gamma)$, where $\ell$ denotes all three lepton flavors, are measured in the following fiducial region: $p_{\mathrm{T}}^{\ell} > 30\,\mathrm{GeV}$, $|\eta^{\ell}| < 2.5$, $p_{\mathrm{T}}^{\gamma} > 30\,\mathrm{GeV}$, $|\eta^{\gamma}| < 2.5$, $p_{\mathrm{T}}^{\mathrm{miss}} > 40\,\mathrm{GeV}$, and $\Delta R(\ell, \gamma) > 0.7$. The leptons are dressed by adding the four-momenta of any photons with $\Delta R(\ell, \gamma) < 0.1$ to the four-momentum of the lepton. A smooth-cone photon isolation is also applied, with parameters $\delta_{0}=0.4$, $\epsilon=1.0$, and $n=1$.
Relative uncertainties on the measured absolute differential $\Delta R(\ell,\gamma)$ cross section.
Relative uncertainties on the measured fractional differential $\Delta R(\ell,\gamma)$ cross section.
Correlation matrix for the measured absolute differential $\Delta R(\ell,\gamma)$ cross section.
Correlation matrix for the measured fractional differential $\Delta R(\ell,\gamma)$ cross section.
Response matrix from the fiducial to the reconstructed bins of the differential $\Delta R(\ell,\gamma)$ cross section measurement.
Measured absolute differential $\Delta\eta(\ell,\gamma)$ cross section, compared to the MG5_aMC+PY8, GENEVA, MATRIX and MCFM predictions. The differential cross sections $\sigma_{j}(\mathrm{pp}\rightarrow\mathrm{W}^{\pm}\gamma\rightarrow\ell^{\pm}\nu\gamma)$, where $\ell$ denotes all three lepton flavors, are measured in the following fiducial region: $p_{\mathrm{T}}^{\ell} > 30\,\mathrm{GeV}$, $|\eta^{\ell}| < 2.5$, $p_{\mathrm{T}}^{\gamma} > 30\,\mathrm{GeV}$, $|\eta^{\gamma}| < 2.5$, $p_{\mathrm{T}}^{\mathrm{miss}} > 40\,\mathrm{GeV}$, and $\Delta R(\ell, \gamma) > 0.7$. The leptons are dressed by adding the four-momenta of any photons with $\Delta R(\ell, \gamma) < 0.1$ to the four-momentum of the lepton. A smooth-cone photon isolation is also applied, with parameters $\delta_{0}=0.4$, $\epsilon=1.0$, and $n=1$.
Measured fractional differential $\Delta\eta(\ell,\gamma)$ cross section, compared to the MG5_aMC+PY8, GENEVA, MATRIX and MCFM predictions. The differential cross sections $\sigma_{j}(\mathrm{pp}\rightarrow\mathrm{W}^{\pm}\gamma\rightarrow\ell^{\pm}\nu\gamma)$, where $\ell$ denotes all three lepton flavors, are measured in the following fiducial region: $p_{\mathrm{T}}^{\ell} > 30\,\mathrm{GeV}$, $|\eta^{\ell}| < 2.5$, $p_{\mathrm{T}}^{\gamma} > 30\,\mathrm{GeV}$, $|\eta^{\gamma}| < 2.5$, $p_{\mathrm{T}}^{\mathrm{miss}} > 40\,\mathrm{GeV}$, and $\Delta R(\ell, \gamma) > 0.7$. The leptons are dressed by adding the four-momenta of any photons with $\Delta R(\ell, \gamma) < 0.1$ to the four-momentum of the lepton. A smooth-cone photon isolation is also applied, with parameters $\delta_{0}=0.4$, $\epsilon=1.0$, and $n=1$.
Relative uncertainties on the measured absolute differential $\Delta \eta(\ell,\gamma)$ cross section.
Relative uncertainties on the measured fractional differential $\Delta \eta(\ell,\gamma)$ cross section.
Correlation matrix for the measured absolute differential $\Delta \eta(\ell,\gamma)$ cross section.
Correlation matrix for the measured fractional differential $\Delta \eta(\ell,\gamma)$ cross section.
Response matrix from the fiducial to the reconstructed bins of the differential $\Delta \eta(\ell,\gamma)$ cross section measurement.
Measured absolute differential $m_{\mathrm{T}}^{\mathrm{cluster}}$ cross section, compared to the MG5_aMC+PY8, GENEVA, MATRIX and MCFM predictions. The differential cross sections $\sigma_{j}(\mathrm{pp}\rightarrow\mathrm{W}^{\pm}\gamma\rightarrow\ell^{\pm}\nu\gamma)$, where $\ell$ denotes all three lepton flavors, are measured in the following fiducial region: $p_{\mathrm{T}}^{\ell} > 30\,\mathrm{GeV}$, $|\eta^{\ell}| < 2.5$, $p_{\mathrm{T}}^{\gamma} > 30\,\mathrm{GeV}$, $|\eta^{\gamma}| < 2.5$, $p_{\mathrm{T}}^{\mathrm{miss}} > 40\,\mathrm{GeV}$, and $\Delta R(\ell, \gamma) > 0.7$. The leptons are dressed by adding the four-momenta of any photons with $\Delta R(\ell, \gamma) < 0.1$ to the four-momentum of the lepton. A smooth-cone photon isolation is also applied, with parameters $\delta_{0}=0.4$, $\epsilon=1.0$, and $n=1$.
Measured fractional differential $m_{\mathrm{T}}^{\mathrm{cluster}}$ cross section, compared to the MG5_aMC+PY8, GENEVA, MATRIX and MCFM predictions. The differential cross sections $\sigma_{j}(\mathrm{pp}\rightarrow\mathrm{W}^{\pm}\gamma\rightarrow\ell^{\pm}\nu\gamma)$, where $\ell$ denotes all three lepton flavors, are measured in the following fiducial region: $p_{\mathrm{T}}^{\ell} > 30\,\mathrm{GeV}$, $|\eta^{\ell}| < 2.5$, $p_{\mathrm{T}}^{\gamma} > 30\,\mathrm{GeV}$, $|\eta^{\gamma}| < 2.5$, $p_{\mathrm{T}}^{\mathrm{miss}} > 40\,\mathrm{GeV}$, and $\Delta R(\ell, \gamma) > 0.7$. The leptons are dressed by adding the four-momenta of any photons with $\Delta R(\ell, \gamma) < 0.1$ to the four-momentum of the lepton. A smooth-cone photon isolation is also applied, with parameters $\delta_{0}=0.4$, $\epsilon=1.0$, and $n=1$.
Relative uncertainties on the measured absolute differential $m_{\mathrm{T}}^{\mathrm{cluster}}$ cross section.
Relative uncertainties on the measured fractional differential $m_{\mathrm{T}}^{\mathrm{cluster}}$ cross section.
Correlation matrix for the measured absolute differential $m_{\mathrm{T}}^{\mathrm{cluster}}$ cross section.
Correlation matrix for the measured fractional differential $m_{\mathrm{T}}^{\mathrm{cluster}}$ cross section.
Response matrix from the fiducial to the reconstructed bins of the differential $m_{\mathrm{T}}^{\mathrm{cluster}}$ cross section measurement.
Measured absolute differential $N_{\mathrm{jets}}$ cross section, compared to the MG5_aMC+PY8, GENEVA, MATRIX and MCFM predictions. The differential cross sections $\sigma_{j}(\mathrm{pp}\rightarrow\mathrm{W}^{\pm}\gamma\rightarrow\ell^{\pm}\nu\gamma)$, where $\ell$ denotes all three lepton flavors, are measured in the following fiducial region: $p_{\mathrm{T}}^{\ell} > 30\,\mathrm{GeV}$, $|\eta^{\ell}| < 2.5$, $p_{\mathrm{T}}^{\gamma} > 30\,\mathrm{GeV}$, $|\eta^{\gamma}| < 2.5$, $p_{\mathrm{T}}^{\mathrm{miss}} > 40\,\mathrm{GeV}$, and $\Delta R(\ell, \gamma) > 0.7$. The leptons are dressed by adding the four-momenta of any photons with $\Delta R(\ell, \gamma) < 0.1$ to the four-momentum of the lepton. A smooth-cone photon isolation is also applied, with parameters $\delta_{0}=0.4$, $\epsilon=1.0$, and $n=1$.
Correlation matrix for the measured absolute differential $N_{\mathrm{jets}}$ cross section. The differential cross sections $\sigma_{j}(\mathrm{pp}\rightarrow\mathrm{W}^{\pm}\gamma\rightarrow\ell^{\pm}\nu\gamma)$, where $\ell$ denotes all three lepton flavors, are measured in the following fiducial region: $p_{\mathrm{T}}^{\ell} > 30\,\mathrm{GeV}$, $|\eta^{\ell}| < 2.5$, $p_{\mathrm{T}}^{\gamma} > 30\,\mathrm{GeV}$, $|\eta^{\gamma}| < 2.5$, $p_{\mathrm{T}}^{\mathrm{miss}} > 40\,\mathrm{GeV}$, and $\Delta R(\ell, \gamma) > 0.7$. The leptons are dressed by adding the four-momenta of any photons with $\Delta R(\ell, \gamma) < 0.1$ to the four-momentum of the lepton. A smooth-cone photon isolation is also applied, with parameters $\delta_{0}=0.4$, $\epsilon=1.0$, and $n=1$.
Response matrix from the fiducial to the reconstructed bins of the differential $N_{\mathrm{jets}}$ cross section measurement.
Relative uncertainties on the measured absolute differential $N_{\mathrm{jets}}$ cross section.
Measured absolute differential $\Delta\eta(\ell,\gamma)$ cross section, compared to the MG5_aMC+PY8, GENEVA, MATRIX and MCFM predictions. The differential cross sections $\sigma_{j}(\mathrm{pp}\rightarrow\mathrm{W}^{\pm}\gamma\rightarrow\ell^{\pm}\nu\gamma)$, where $\ell$ denotes all three lepton flavors, are measured in the following fiducial region: $p_{\mathrm{T}}^{\ell} > 30\,\mathrm{GeV}$, $|\eta^{\ell}| < 2.5$, $p_{\mathrm{T}}^{\gamma} > 30\,\mathrm{GeV}$, $|\eta^{\gamma}| < 2.5$, $p_{\mathrm{T}}^{\mathrm{miss}} > 40\,\mathrm{GeV}$, and $\Delta R(\ell, \gamma) > 0.7$. The leptons are dressed by adding the four-momenta of any photons with $\Delta R(\ell, \gamma) < 0.1$ to the four-momentum of the lepton. A smooth-cone photon isolation is also applied, with parameters $\delta_{0}=0.4$, $\epsilon=1.0$, and $n=1$. Requirements of $m_{\mathrm{T}}^{\mathrm{cluster}}>150\,\mathrm{GeV}$ and a veto on the presence of any jet with $p_{\mathrm{T}} > 30\,\mathrm{GeV}$ and $|\eta| < 2.5$ are applied in addition to the baseline selection.
Measured fractional differential $\Delta\eta(\ell,\gamma)$ cross section, compared to the MG5_aMC+PY8, GENEVA, MATRIX and MCFM predictions. The differential cross sections $\sigma_{j}(\mathrm{pp}\rightarrow\mathrm{W}^{\pm}\gamma\rightarrow\ell^{\pm}\nu\gamma)$, where $\ell$ denotes all three lepton flavors, are measured in the following fiducial region: $p_{\mathrm{T}}^{\ell} > 30\,\mathrm{GeV}$, $|\eta^{\ell}| < 2.5$, $p_{\mathrm{T}}^{\gamma} > 30\,\mathrm{GeV}$, $|\eta^{\gamma}| < 2.5$, $p_{\mathrm{T}}^{\mathrm{miss}} > 40\,\mathrm{GeV}$, and $\Delta R(\ell, \gamma) > 0.7$. The leptons are dressed by adding the four-momenta of any photons with $\Delta R(\ell, \gamma) < 0.1$ to the four-momentum of the lepton. A smooth-cone photon isolation is also applied, with parameters $\delta_{0}=0.4$, $\epsilon=1.0$, and $n=1$. Requirements of $m_{\mathrm{T}}^{\mathrm{cluster}}>150\,\mathrm{GeV}$ and a veto on the presence of any jet with $p_{\mathrm{T}} > 30\,\mathrm{GeV}$ and $|\eta| < 2.5$ are applied in addition to the baseline selection.
Relative uncertainties on the measured absolute differential $\Delta \eta(\ell,\gamma)$ cross section. Requirements of $m_{\mathrm{T}}^{\mathrm{cluster}}>150\,\mathrm{GeV}$ and a veto on the presence of any jet with $p_{\mathrm{T}} > 30\,\mathrm{GeV}$ and $|\eta| < 2.5$ are applied in addition to the baseline selection.
Relative uncertainties on the measured fractional differential $\Delta \eta(\ell,\gamma)$ cross section. Requirements of $m_{\mathrm{T}}^{\mathrm{cluster}}>150\,\mathrm{GeV}$ and a veto on the presence of any jet with $p_{\mathrm{T}} > 30\,\mathrm{GeV}$ and $|\eta| < 2.5$ are applied in addition to the baseline selection.
Correlation matrix for the measured absolute differential $\Delta \eta(\ell,\gamma)$ cross section. Requirements of $m_{\mathrm{T}}^{\mathrm{cluster}}>150\,\mathrm{GeV}$ and a veto on the presence of any jet with $p_{\mathrm{T}} > 30\,\mathrm{GeV}$ and $|\eta| < 2.5$ are applied in addition to the baseline selection.
Correlation matrix for the measured fractional differential $\Delta \eta(\ell,\gamma)$ cross section. Requirements of $m_{\mathrm{T}}^{\mathrm{cluster}}>150\,\mathrm{GeV}$ and a veto on the presence of any jet with $p_{\mathrm{T}} > 30\,\mathrm{GeV}$ and $|\eta| < 2.5$ are applied in addition to the baseline selection.
Response matrix from the fiducial to the reconstructed bins of the differential $\Delta \eta(\ell,\gamma)$ cross section measurement. Requirements of $m_{\mathrm{T}}^{\mathrm{cluster}}>150\,\mathrm{GeV}$ and a veto on the presence of any jet with $p_{\mathrm{T}} > 30\,\mathrm{GeV}$ and $|\eta| < 2.5$ are applied in addition to the baseline selection.
Fiducial cross section scaling terms as a function of $C_{3W}$ in all $p_{\mathrm{T}}^{\gamma} \times |\phi_{f}|$ bins. Values are given relative to the SM prediction.
Scans of the profile likelihood test statistic $q$ as a function of $C_{3W}$, given with and without the pure BSM term.
Scans of the profile likelihood test statistic $q$ as a function of $C_{3W}$, given with and without the pure BSM term.
Best-fit values of $C_{3W}$ and corresponding 95% CL confidence intervals as a function of the maximum $p_{\mathrm{T}}^{\gamma}$ bin included in the fit, with and without the pure BSM term.
Best-fit values of $C_{3W}$ and corresponding 95% CL confidence intervals as a function of the maximum $p_{\mathrm{T}}^{\gamma}$ bin included in the fit, with and without the binning in $|\phi_{f}|$.
Response matrix from the fiducial to the reconstructed bins of the differential $p_{\mathrm{T}}^{\gamma} \times |\phi_{f}|$ cross section measurement.
Measured double-differential $p_{\mathrm{T}}^{\gamma} \times |\phi_{f}|$ cross section, compared to the MG5_aMC+PY8 NLO prediction. The differential cross sections $\sigma_{j}(\mathrm{pp}\rightarrow\mathrm{W}^{\pm}\gamma\rightarrow\ell^{\pm}\nu\gamma)$, where $\ell$ denotes all three lepton flavors, are measured in the following fiducial region: $p_{\mathrm{T}}^{\ell} > 80\,\mathrm{GeV}$, $|\eta^{\ell}| < 2.5$, $p_{\mathrm{T}}^{\gamma} > 150\,\mathrm{GeV}$, $|\eta^{\gamma}| < 2.5$, $p_{\mathrm{T}}^{\mathrm{miss}} > 40\,\mathrm{GeV}$, and $\Delta R(\ell, \gamma) > 0.7$. The leptons are dressed by adding the four-momenta of any photons with $\Delta R(\ell, \gamma) < 0.1$ to the four-momentum of the lepton. A smooth-cone photon isolation is also applied, with parameters $\delta_{0}=0.4$, $\epsilon=1.0$, and $n=1$. A veto on the presence of any jet with $p_{\mathrm{T}} > 30\,\mathrm{GeV}$ and $|\eta| < 2.5$ is also applied for this result.
Measured double-differential $p_{\mathrm{T}}^{\gamma} \times |\phi_{f}|$ cross section, compared to the MG5_aMC+PY8 NLO prediction. This table gives the entries for the $(0,\pi/6)$ slice. The differential cross sections $\sigma_{j}(\mathrm{pp}\rightarrow\mathrm{W}^{\pm}\gamma\rightarrow\ell^{\pm}\nu\gamma)$, where $\ell$ denotes all three lepton flavors, are measured in the following fiducial region: $p_{\mathrm{T}}^{\ell} > 80\,\mathrm{GeV}$, $|\eta^{\ell}| < 2.5$, $p_{\mathrm{T}}^{\gamma} > 150\,\mathrm{GeV}$, $|\eta^{\gamma}| < 2.5$, $p_{\mathrm{T}}^{\mathrm{miss}} > 40\,\mathrm{GeV}$, and $\Delta R(\ell, \gamma) > 0.7$. The leptons are dressed by adding the four-momenta of any photons with $\Delta R(\ell, \gamma) < 0.1$ to the four-momentum of the lepton. A smooth-cone photon isolation is also applied, with parameters $\delta_{0}=0.4$, $\epsilon=1.0$, and $n=1$. A veto on the presence of any jet with $p_{\mathrm{T}} > 30\,\mathrm{GeV}$ and $|\eta| < 2.5$ is also applied for this result.
Measured double-differential $p_{\mathrm{T}}^{\gamma} \times |\phi_{f}|$ cross section, compared to the MG5_aMC+PY8 NLO prediction. This table gives the entries for the $(\pi/6,\pi/3)$ slice. The differential cross sections $\sigma_{j}(\mathrm{pp}\rightarrow\mathrm{W}^{\pm}\gamma\rightarrow\ell^{\pm}\nu\gamma)$, where $\ell$ denotes all three lepton flavors, are measured in the following fiducial region: $p_{\mathrm{T}}^{\ell} > 80\,\mathrm{GeV}$, $|\eta^{\ell}| < 2.5$, $p_{\mathrm{T}}^{\gamma} > 150\,\mathrm{GeV}$, $|\eta^{\gamma}| < 2.5$, $p_{\mathrm{T}}^{\mathrm{miss}} > 40\,\mathrm{GeV}$, and $\Delta R(\ell, \gamma) > 0.7$. The leptons are dressed by adding the four-momenta of any photons with $\Delta R(\ell, \gamma) < 0.1$ to the four-momentum of the lepton. A smooth-cone photon isolation is also applied, with parameters $\delta_{0}=0.4$, $\epsilon=1.0$, and $n=1$. A veto on the presence of any jet with $p_{\mathrm{T}} > 30\,\mathrm{GeV}$ and $|\eta| < 2.5$ is also applied for this result.
Measured double-differential $p_{\mathrm{T}}^{\gamma} \times |\phi_{f}|$ cross section, compared to the MG5_aMC+PY8 NLO prediction. This table gives the entries for the $(\pi/3,\pi/2)$ slice. The differential cross sections $\sigma_{j}(\mathrm{pp}\rightarrow\mathrm{W}^{\pm}\gamma\rightarrow\ell^{\pm}\nu\gamma)$, where $\ell$ denotes all three lepton flavors, are measured in the following fiducial region: $p_{\mathrm{T}}^{\ell} > 80\,\mathrm{GeV}$, $|\eta^{\ell}| < 2.5$, $p_{\mathrm{T}}^{\gamma} > 150\,\mathrm{GeV}$, $|\eta^{\gamma}| < 2.5$, $p_{\mathrm{T}}^{\mathrm{miss}} > 40\,\mathrm{GeV}$, and $\Delta R(\ell, \gamma) > 0.7$. The leptons are dressed by adding the four-momenta of any photons with $\Delta R(\ell, \gamma) < 0.1$ to the four-momentum of the lepton. A smooth-cone photon isolation is also applied, with parameters $\delta_{0}=0.4$, $\epsilon=1.0$, and $n=1$. A veto on the presence of any jet with $p_{\mathrm{T}} > 30\,\mathrm{GeV}$ and $|\eta| < 2.5$ is also applied for this result.
Correlation matrix for the measured absolute differential $p_{\mathrm{T}}^{\gamma} \times |\phi_{f}|$ cross section.
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