Abstract

We study inclusive jet suppression and modifications in the quark-gluon plasma (QGP) with a transport-based model. The model includes vacuum-like parton shower evolution at high-virtuality, a linearized transport for jet-medium interactions, and a simple ansatz for the jet-induced hydrodynamic response of the medium. Model parameters are calibrated to nuclear modification factors for inclusive hadron {R}_{AA}^h and single inclusive jets {R}_{AA}^j with cone size R = 0.4 in 0–10% central Au-Au and Pb-Pb collisions measured at the RHIC and LHC. The calibrated model consistently describes the cone-size dependent {R}_{AA}^j (R), modifications to inclusive jet fragmentation functions and jet shape. We discuss the origin of these modifications by analyzing the medium-induced jet energy flow in this model and elucidate the interplay of hard parton evolution and jet-induced medium response. In particular, we demonstrate that the excess of soft hadrons at pT∼ 2 GeV/c in jet fragmentation function and jet shape at large r=sqrt{Delta {eta}^2+Delta {phi}^2} are consequences of both soft medium-induced gluon radiation and jet-induced medium excitation.

Highlights

  • Years at both the RHIC and the LHC energies [10]

  • Model parameters are calibrated to nuclear modification factors for inclusive hadron RAh A and single inclusive jets RAj A with cone size R = 0.4 in 0–10% central Au-Au and Pb-Pb collisions measured at the RHIC and LHC

  • As the first work applying this model to jet quenching phenomenology, we only vary a subset of all possible parameters in the model

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Summary

A transport-based model for jet evolution in nuclear collisions

We introduce the jet evolution model that has been outlined in the introduction. The initial hard processes of jet production and vacuum-like evolution of parton shower from Q ∼ phTard to Q = Q0 is modeled by Pythia. 2. The initial jet shower parton production is followed by partons-medium interactions, which are treated in a previously developed linearized partonic transport model LIDO. Jet partons excite the medium in two ways: medium partons that acquire a hard recoiled momentum in collisions with jet partons; the perturbed soft medium partons seed a linearized hydrodynamic-like response. 3. A stage of vacuum evolution of parton shower starting from the virtuality scale acquired in the last parton radiation k⊥,final to ΛQCD occurs outside the QGP medium. A stage of vacuum evolution of parton shower starting from the virtuality scale acquired in the last parton radiation k⊥,final to ΛQCD occurs outside the QGP medium It is followed by hadronization and particle decays. Details of the medium evolution model can be found in appendix A

Jet evolution in vacuum and initialization of transport equation
The LIDO transport model
Medium excitations induced by hard partons: an approximate treatment
Model calibration
Summary of parameters
Experimental dataset
Parameter sets for central prediction and error estimation
Energy flow induced by jet-medium interaction
Energy transport via vacuum and induced radiations
Remarks on trigger bias
Prediction of jet modifications
Modified jet fragmentation function in central Pb-Pb collisions
Cone-size dependence of jet suppression and jet-shape modifications
Summary and outlook
A Medium evolution
B Comparisons of single-gluon emission rates
Procedures of Bayesian parameter calibration
Findings
Sensitivity to the phTadron cut on hadron suppression data
Full Text
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