Energy loss of heavy quarks in the isotropic collisional hot QCD medium

Abstract The collisional energy loss of heavy partons (charm and bottom quarks) has been determined within the framework of semi-classical transport theory implying the Bhatnagar–Gross–Krook (BGK) collisional kernel. Hot QCD medium effects have been incorporated while employing a quasi-particle desc...

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Main Authors: M. Yousuf Jamal, Vinod Chandra
Format: Article
Language:English
Published: SpringerOpen 2019-09-01
Series:European Physical Journal C: Particles and Fields
Online Access:http://link.springer.com/article/10.1140/epjc/s10052-019-7278-2
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spelling doaj-a6c457d16f7447f2b6d3bd16933c89ac2020-11-25T03:25:29ZengSpringerOpenEuropean Physical Journal C: Particles and Fields1434-60441434-60522019-09-017991810.1140/epjc/s10052-019-7278-2Energy loss of heavy quarks in the isotropic collisional hot QCD mediumM. Yousuf Jamal0Vinod Chandra1Indian Institute of Technology GandhinagarIndian Institute of Technology GandhinagarAbstract The collisional energy loss of heavy partons (charm and bottom quarks) has been determined within the framework of semi-classical transport theory implying the Bhatnagar–Gross–Krook (BGK) collisional kernel. Hot QCD medium effects have been incorporated while employing a quasi-particle description of the medium in terms of effective gluons, quarks and antiquarks with respective temperature dependent effective fugacities. The momentum dependence of the energy loss for the charm and the bottom quark has been investigated. It is observed that with the increase in momentum of the heavy quarks, the loss increases sharply for the smaller values and reaches saturation later. Furthermore, as compared to the charm quark, the bottom quark loses less energy at a particular momentum and collisional frequency. The energy loss is seen to increase with increasing collisional frequency. We also provide a comparative study of the results obtained using the BGK kernel rather than those using the relaxation time approximation (RTA) kernel and found them to be consistent with each other. The medium effects in all the situations are seen to play a quite significant role.http://link.springer.com/article/10.1140/epjc/s10052-019-7278-2
collection DOAJ
language English
format Article
sources DOAJ
author M. Yousuf Jamal
Vinod Chandra
spellingShingle M. Yousuf Jamal
Vinod Chandra
Energy loss of heavy quarks in the isotropic collisional hot QCD medium
European Physical Journal C: Particles and Fields
author_facet M. Yousuf Jamal
Vinod Chandra
author_sort M. Yousuf Jamal
title Energy loss of heavy quarks in the isotropic collisional hot QCD medium
title_short Energy loss of heavy quarks in the isotropic collisional hot QCD medium
title_full Energy loss of heavy quarks in the isotropic collisional hot QCD medium
title_fullStr Energy loss of heavy quarks in the isotropic collisional hot QCD medium
title_full_unstemmed Energy loss of heavy quarks in the isotropic collisional hot QCD medium
title_sort energy loss of heavy quarks in the isotropic collisional hot qcd medium
publisher SpringerOpen
series European Physical Journal C: Particles and Fields
issn 1434-6044
1434-6052
publishDate 2019-09-01
description Abstract The collisional energy loss of heavy partons (charm and bottom quarks) has been determined within the framework of semi-classical transport theory implying the Bhatnagar–Gross–Krook (BGK) collisional kernel. Hot QCD medium effects have been incorporated while employing a quasi-particle description of the medium in terms of effective gluons, quarks and antiquarks with respective temperature dependent effective fugacities. The momentum dependence of the energy loss for the charm and the bottom quark has been investigated. It is observed that with the increase in momentum of the heavy quarks, the loss increases sharply for the smaller values and reaches saturation later. Furthermore, as compared to the charm quark, the bottom quark loses less energy at a particular momentum and collisional frequency. The energy loss is seen to increase with increasing collisional frequency. We also provide a comparative study of the results obtained using the BGK kernel rather than those using the relaxation time approximation (RTA) kernel and found them to be consistent with each other. The medium effects in all the situations are seen to play a quite significant role.
url http://link.springer.com/article/10.1140/epjc/s10052-019-7278-2
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