A model of jet quenching in ultrarelativistic heavy ion collisionsand high- pT hadron spectra at RHIC

By I. Lokhtin, A. Snigirev. 2005

388 citations recorded by the source corpus.

Abstract.The method to simulate the rescattering and energy loss of hard partons in ultrarelativistic heavy ion collisions has been developed. The model is a fast Monte Carlo tool introduced to modify a standard PYTHIA jet event. The full heavy ion event is obtained as a superposition of a soft hydro-type state and hard multi-jets. The model is applied to the analysis of the jet quenching pattern at RHIC.

Subfields: Nuclear and High Energy Physics

View Paper: https://www.semanticscholar.org/paper/1536978d1b75a8563fc63dce6a41576a8c7289f1

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In Nuclear and High Energy Physics

Citations in the corpus

The CMS trigger system (2004, methodology): “The selection efficiency of this trigger was determined using a MC simulation of HI events using the hydjet event generator [60] and was cross-checked with a control data sample selected using the BPTX signal to identify crossing beam bunches.”
Study of high-pT charged particle suppression in PbPb compared to pp collisions at sqrt(sNN)=2.76 TeV (2012, methodology): “To improve the statistical precision of the correction factors at high pT, HYDJET MC samples are also mixed at the level of simulated hits with dijet events generated with different settings of the hard-scattering scale (p̂T=30, 50, 80, 110, and 170 GeV/c) from PYQUEN [17], a generator for the simul”
Modification of jet shapes in PbPb collisions at √sNN=2.76TeV (2014, methodology): “In order to account for the influence of the underlying PbPb events, the pythia events are embedded into fully simulated PbPb events, generated by hydjet [42] (version 1.”
Measurement of jet fragmentation in PbPb and pp collisions at s NN =2.76 TeV (2014, methodology): “The quoted systematic uncertainty band is cross-checked by repeating the complete analysis with PYTHIA + HYDJET corrections applied to reconstructed events in which quenched jets generated using PYQUEN [27] are embedded.”
Observation and studies of jet quenching in PbPb collisions at nucleon-nucleon center-of-mass energy = 2.76 TeV (2011, methodology): “The HYDJET events included the simulation of hard-scattering processes for which radiative parton energy loss was simulated, but collisional energy loss was turned off [42].”
Study of high-pT charged particle suppression in PbPb compared to pp collisions at $\sqrt{s_{\mathrm{NN}}}=2.76~\mathrm{TeV}$ (2012, methodology): “To improve the statistical precision of the correction factors at high pT, HYDJET MC samples are also mixed at the level of simulated hits with dijet events generated with different settings of the hard-scattering scale (p̂T=30, 50, 80, 110, and 170 GeV/c) from PYQUEN [17], a generator for the simul”
Measurement of nuclear modification factors of ϒ(1S), ϒ(2S), and ϒ(3S) mesons in PbPb collisions at sNN=5.02 TeV (2018, neutral): “9 for the PbPb events [38].”