Abstract

Within perturbative QCD, we develop a new picture for the parton shower generated by a jet propagating through a dense quark-gluon plasma. This picture combines in a simple, factorised, way multiple medium-induced parton branchings and standard vacuum-like emissions, with the phase-space for the latter constrained by the presence of the medium. We implement this picture as a Monte Carlo generator that we use to study two phenomenologically important observables: the jet nuclear modification factor RAA and the \U0001d4cfg distribution reflecting the jet substructure. In both cases, the outcome of our Monte Carlo simulations is in good agreement with the LHC measurements. We provide basic analytic calculations that help explaining the main features observed in the data. We find that the energy loss by the jet is increasing with the jet transverse momentum, due to a rise in the number of partonic sources via vacuum-like emissions. This is a key element in our description of both RAA and the \U0001d4cfg distribution. For the latter, we identify two main nuclear effects: incoherent jet energy loss and hard medium-induced emissions. As the jet transverse momentum increases, we predict a qualitative change in the ratio between the \U0001d4cfg distributions in PbPb and pp collisions: from increasing at small \U0001d4cfg, this ratio becomes essentially flat, or even slightly decreasing.

Highlights

  • ArXiv ePrint: 1907.04866 We want to dedicate this paper to the 80th birthday of Al Mueller, who pioneered the studies of jet quenching in perturbative QCD and was our collaborator on a previous paper which introduced the general physical picture that we further develop in this work

  • The main lessons one draws from our study of high-energy jets are as follows: (i) the incoherent energy loss by the two subjets created by the hard splitting leads to a suppression in the nuclear zg distribution which is larger at small zg; (ii) the MC results are sensitive to the evolution of the subjets multiplicity via vacuum-like emissions (VLEs) which leads to an energy loss increasing with the subjet pT ; (iii) this last effect may be hidden when studying the self-normalised zg distribution; in that respect, the Njets-normalised distribution is better suited to disentangle between different energy-loss models

  • We have presented a new picture, emerging from perturbative QCD, for the parton shower created by an energetic parton propagating through a dense quark-gluon plasma

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Summary

Parton shower in the medium: physical picture

We describe our factorised pQCD picture for the parton shower generated by an energetic parton propagating through a homogeneous dense QCD medium of size L. We discuss the validity of this picture beyond the double-logarithmic approximation originally used in ref. [27]

Basic considerations
Factorisation of vacuum-like emissions in the presence of the medium
A single-logarithmic approximation with angular ordering
Medium-induced radiation
Transverse momentum broadening
Energy loss by the jet: medium-induced emissions only
Energy loss by the jet: full parton shower
Parton shower in the medium
Limitations
Energy loss by the jet and the nuclear modification factor
The average energy loss by the jet
The nuclear modification factor RAA
General definitions and zg in the vacuum
In-medium zg distribution
Analytic insight for high-energy jets
Analytic insight for low-energy jets
Low-energy jets: medium-induced emissions only
L 2ω2θ ω2θ2
Low-energy jets: energy loss only
Low-energy jets: full parton showers
Phenomenology with the Njets-normalised zg
Self-normalised zg distribution and CMS data
Substructure observables beyond the zg distribution
Findings
Conclusions and perspectives
Full Text
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