13–16 Jan 2025
Asia/Kolkata timezone

Investigations of event-by-event fluctuations of mean transverse momentum ($\langle p_{\rm T} \rangle$) in pp collisions at $\sqrt{s}$= 13 TeV with PYTHIA8 and HERWIG7 models

15 Jan 2025, 12:08
7m
1. QCD Phase Diagram, criticality and fluctuations Parallel C

Speaker

Subhadeep Roy (IIT- Indian Institute of Technology (IN))

Description

The study of event-by-event mean transverse momentum ($\langle p_{\rm T} \rangle$) fluctuations is reported in terms of the integral two-particle correlator ($\langle \Delta p_{\rm T} \Delta p_{\rm T}\rangle$) and skewness of the event-wise $\langle p_{\rm T} \rangle$ distribution in proton$-$proton (pp) collisions at $\sqrt{s}=13$ TeV. The simulations were carried out using the Monte Carlo event generators PYTHIA8 and HERWIG7. Charged particles with transverse momentum ($p_{\rm T}$) and pseudo-rapidity ($\eta$) ranges $0.15 \leq p_{\rm T}\leq 2.0$ GeV/$c$ and $|\eta| \leq 0.8$ were taken into the consideration. The correlator $\langle \Delta p_{\rm T} \Delta p_{\rm T}\rangle$ is observed to follow distinct declining trends with the average charged particle multiplicity ($\langle N_{\rm ch} \rangle$) for PYTHIA8 and HERWIG7 models. Furthermore, both models yield positive finite skewness in low-multiplicity events. The observables are additionally studied using the transverse spherocity estimator ($S_{\rm 0}$) to comprehend the relative contributions of hard scattering (jets) and soft multi-partonic interactions (MPI) to the observed fluctuations. The comparative measurements using these models would help in understanding the fluctuation dynamics and constraint the particle productions in such models.

Authors

Sadhana Dash (IIT- Indian Institute of Technology (IN)) Subhadeep Roy (IIT- Indian Institute of Technology (IN)) Tanu Gahlaut (IIT- Indian Institute of Technology (IN))

Presentation materials