Measurement of the nuclear modification factor of b-jets in 5.02 TeV Pb+Pb collisions with the ATLAS detector
dc.contributor.author | Aad G. | |
dc.contributor.author | Abbott B. | |
dc.contributor.author | Abbott D. C. | |
dc.contributor.author | Abeling K. | |
dc.contributor.author | Abidi S. H. | |
dc.contributor.author | Aboulhorma A. | |
dc.contributor.author | Abramowicz H. | |
dc.contributor.author | Abreu H. | |
dc.contributor.author | Abulaiti Y. | |
dc.contributor.author | Abusleme Hoffman A. C. | |
dc.contributor.author | Acharya B. S. | |
dc.contributor.author | Achkar B. | |
dc.contributor.author | Adam L. | |
dc.contributor.author | Adam Bourdarios C. | |
dc.contributor.author | Adamczyk L. | |
dc.contributor.author | Adamek L. | |
dc.contributor.author | Addepalli S. V. | |
dc.contributor.author | Adelman J. | |
dc.contributor.author | Adiguzel A. | |
dc.contributor.author | Adorni S. | |
dc.contributor.author | Adye T. | |
dc.contributor.author | Affolder A. A. | |
dc.contributor.author | Afik Y. | |
dc.contributor.author | Agaras M. N. | |
dc.contributor.author | Agarwala J. | |
dc.contributor.author | Aggarwal A. | |
dc.contributor.author | Agheorghiesei C. | |
dc.contributor.author | Aguilar-Saavedra J. A. | |
dc.contributor.author | Ahmad A. | |
dc.contributor.author | Ahmadov F. | |
dc.contributor.author | Ahmed W. S. | |
dc.contributor.author | Ai X. | |
dc.contributor.author | Aielli G. | |
dc.contributor.author | Aizenberg I. | |
dc.contributor.author | Akbiyik M. | |
dc.contributor.author | Akesson T. P. A. | |
dc.contributor.author | Akimov A. V. | |
dc.contributor.author | Al Khoury K. | |
dc.contributor.author | Alberghi G. L. | |
dc.contributor.author | Albert J. | |
dc.date.accessioned | 2025-05-19T16:37:49Z | |
dc.date.available | 2025-05-19T16:37:49Z | |
dc.date.issued | 2023/05/25 | |
dc.description.abstract | This paper presents a measurement of b-jet production in Pb+Pb and pp collisions at root s(NN) = 5.02 TeV with the ATLAS detector at the LHC. The measurement uses 260 pb(-1) of pp collisions collected in 2017 and 1.4 nb(-1) of Pb+Pb collisions collected in 2018. In both collision systems, jets are reconstructed via the anti-kt algorithm. The b-jets are identified from a sample of jets containing muons from the semileptonic decay of b-quarks using template fits of the muon momentum relative to the jet axis. In pp collisions, b-jets are reconstructed for radius parameters R=0.2 and R=0.4, and only R=0.2 jets are used in Pb+Pb collisions. For comparison, inclusive R=0.2 jets are also measured using 1.7 nb(-1) of Pb+Pb collisions collected in 2018 and the same pp collision data as the b-jet measurement. The nuclear modification factor, RAA, is calculated for both b-jets and inclusive jets with R=0.2 over the transverse momentum range of 80-290 GeV. The nuclear modification factor for b-jets decreases from peripheral to central collisions. The ratio of the b-jet RAA to inclusive jet RAA is also presented and suggests that the RAA for b-jets is larger than that for inclusive jets in central Pb+Pb collisions. The measurements are compared with theoretical calculations and suggest a role for mass and colour-charge effects in partonic energy loss in heavy-ion collisions. | |
dc.identifier.doi | http://dx.doi.org/10.1140/epjc/s10052-023-11427-9 | |
dc.identifier.issn | 1434-6044 | |
dc.identifier.uri | https://publicacionesabiertas.userena.cl/handle/123456789/217 | |
dc.language | English | |
dc.publisher | SPRINGER | |
dc.title | Measurement of the nuclear modification factor of b-jets in 5.02 TeV Pb+Pb collisions with the ATLAS detector | |
dc.type | Article |