Production of pions, kaons, and protons as a function of the relative transverse activity classifier in pp collisions at $\sqrt{s}=13$ TeV

Description
Figures from paper submitted to Journal of High Energy Physics
Abstract:

The production of $\pi^\pm$, ${\rm K}^\pm$, and $(\overline{\rm p})$p is measured in pp collisions at $\sqrt{s}=13$ TeV in different topological regions. Particle transverse momentum ($p_{\rm T}$) spectra are measured in the ``toward'', ``transverse'', and ``away'' angular regions defined with respect to the direction of the leading particle in the event. While the toward and away regions contain the fragmentation products of the near-side and away-side jets, respectively, the transverse region is dominated by particles from the Underlying Event (UE). The relative transverse activity classifier, $R_{\rm T}=N_{\rm T}/\langle N_{\rm T}\rangle$, is used to group events according to their UE activity, where $N_{\rm T}$ is the measured charged-particle multiplicity per event in the transverse region and $\langle N_{\rm T}\rangle$ is the mean value over all the analysed events. The first measurements of identified particle $p_{\rm T}$ spectra as a function of $R_{\rm T}$ in the three topological regions are reported. The yield of high transverse momentum particles relative to the $R_{\rm T}$-integrated measurement decreases with increasing $R_{\rm T}$ in both the toward and away regions, indicating that the softer UE dominates particle production as $R_{\rm T}$ increases and validating that $R_{\rm T}$ can be used to control the magnitude of the UE. Conversely, the spectral shapes in the transverse region harden significantly with increasing $R_{\rm T}$. This hardening follows a mass ordering, being more significant for heavier particles. The $p_{\rm T}$-differential particle ratios $({\rm p+\overline{p}})/(\pi^+ +\pi^-)$ and $({\rm K^+ +K^-})/(\pi^+ +\pi^-)$ in the low UE limit $(R_{\rm T}\rightarrow 0)$ approach expectations from Monte Carlo generators such as PYTHIA 8 with Monash 2013 tune and EPOS LHC, where the jet-fragmentation models have been tuned to reproduce ${\rm e^+ e^-}$ results.

JHEP 06 (2023) 027
e-Print: arXiv:2301.10120 | PDF | inSPIRE

Paper:

Energy
13 TeV
System
p-p
Scope: PWG
PWG-MM (Monte Carlo generators and Minimum Bias)
Figure image (.eps)
Energy
13 TeV
System
p-p
Scope: PWG
PWG-MM (Monte Carlo generators and Minimum Bias)
Figure image (.eps)
Energy
13 TeV
System
p-p
Scope: PWG
PWG-MM (Monte Carlo generators and Minimum Bias)
Figure image (.eps)
Energy
13 TeV
System
p-p
Scope: PWG
PWG-MM (Monte Carlo generators and Minimum Bias)
Figure image (.eps)
Energy
13 TeV
System
p-p
Scope: PWG
PWG-MM (Monte Carlo generators and Minimum Bias)
Figure image (.eps)
Energy
13 TeV
System
p-p
Scope: PWG
PWG-MM (Monte Carlo generators and Minimum Bias)
Figure image (.eps)
Energy
13 TeV
System
p-p
Scope: PWG
PWG-MM (Monte Carlo generators and Minimum Bias)
Figure image (.eps)
Energy
13 TeV
System
p-p
Scope: PWG
PWG-MM (Monte Carlo generators and Minimum Bias)
Figure image (.eps)
Energy
13 TeV
System
p-p
Scope: PWG
PWG-MM (Monte Carlo generators and Minimum Bias)
Figure image (.eps)
Energy
13 TeV
System
p-p
Scope: PWG
PWG-MM (Monte Carlo generators and Minimum Bias)
Figure image (.eps)
Energy
13 TeV
System
p-p
Scope: PWG
PWG-MM (Monte Carlo generators and Minimum Bias)
Energy
13 TeV
System
p-p
Scope: PWG
PWG-MM (Monte Carlo generators and Minimum Bias)
Energy
13 TeV
System
p-p
Scope: PWG
PWG-MM (Monte Carlo generators and Minimum Bias)
Energy
13 TeV
System
p-p
Scope: PWG
PWG-MM (Monte Carlo generators and Minimum Bias)
Figure image (.eps)
Energy
13 TeV
System
p-p
Scope: PWG
PWG-MM (Monte Carlo generators and Minimum Bias)
Figure image (.eps)