Charged-particle nuclear modification factors in XeXe collisions at √sNN=5.44 TeV

The differential yields of charged particles having pseudorapidity within |η| < 1 are measured using xenon-xenon (XeXe) collisions at √sNN = 5.44 TeV. The data, corresponding to an integrated luminosity of 3.42 µb −1 , were collected in 2017 by the CMS experiment at the LHC. The yields are re...

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Main Authors: Sirunyan, A. M., Tumasyan, A. R., Adam, Wolfgang, Ambrogi, Federico, Asilar, Ece, Md. Ali, Mohd. Adli
Format: Article
Language:English
English
English
Published: Springer Verlag 2018
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http://irep.iium.edu.my/70212/13/70212_Charged-particle%20nuclear%20modification%20factors_WOS.pdf
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https://link.springer.com/content/pdf/10.1007%2FJHEP10%282018%29138.pdf
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spelling my.iium.irep.702122019-07-15T01:38:57Z http://irep.iium.edu.my/70212/ Charged-particle nuclear modification factors in XeXe collisions at √sNN=5.44 TeV Sirunyan, A. M. Tumasyan, A. R. Adam, Wolfgang Ambrogi, Federico Asilar, Ece Md. Ali, Mohd. Adli Q Science (General) QC Physics The differential yields of charged particles having pseudorapidity within |η| < 1 are measured using xenon-xenon (XeXe) collisions at √sNN = 5.44 TeV. The data, corresponding to an integrated luminosity of 3.42 µb −1 , were collected in 2017 by the CMS experiment at the LHC. The yields are reported as functions of collision centrality and transverse momentum, pT, from 0.5 to 100 GeV. A previously reported pT spectrum from proton-proton collisions at √ s = 5.02 TeV is used for comparison after correcting for the difference in center-of-mass energy. The nuclear modification factors using this reference, R∗ AA, are constructed and compared to previous measurements and theoretical predictions. In head-on collisions, the R∗ AA has a value of 0.17 in the pT range of 6–8 GeV, but increases to approximately 0.7 at 100 GeV. Above ≈6 GeV, the XeXe data show a notably smaller suppression than previous results for lead-lead (PbPb) collisions at √sNN = 5.02 TeV when compared at the same centrality (i.e., the same fraction of total cross section). However, the XeXe suppression is slightly greater than that for PbPb in events having a similar number of participating nucleons. Springer Verlag 2018-10-01 Article NonPeerReviewed application/pdf en http://irep.iium.edu.my/70212/1/70212_Charged-particle%20nuclear%20modification%20factors%20in%20XeXe_article_new.pdf application/pdf en http://irep.iium.edu.my/70212/2/70212_Charged-particle%20nuclear%20modification%20factors%20in%20XeXe_scopus.pdf application/pdf en http://irep.iium.edu.my/70212/13/70212_Charged-particle%20nuclear%20modification%20factors_WOS.pdf Sirunyan, A. M. and Tumasyan, A. R. and Adam, Wolfgang and Ambrogi, Federico and Asilar, Ece and Md. Ali, Mohd. Adli (2018) Charged-particle nuclear modification factors in XeXe collisions at √sNN=5.44 TeV. Journal of High Energy Physics, 2018 (10). pp. 1-41. ISSN 1029-8479 https://link.springer.com/content/pdf/10.1007%2FJHEP10%282018%29138.pdf 10.1007/JHEP10(2018)138
institution Universiti Islam Antarabangsa Malaysia
building IIUM Library
collection Institutional Repository
continent Asia
country Malaysia
content_provider International Islamic University Malaysia
content_source IIUM Repository (IREP)
url_provider http://irep.iium.edu.my/
language English
English
English
topic Q Science (General)
QC Physics
spellingShingle Q Science (General)
QC Physics
Sirunyan, A. M.
Tumasyan, A. R.
Adam, Wolfgang
Ambrogi, Federico
Asilar, Ece
Md. Ali, Mohd. Adli
Charged-particle nuclear modification factors in XeXe collisions at √sNN=5.44 TeV
description The differential yields of charged particles having pseudorapidity within |η| < 1 are measured using xenon-xenon (XeXe) collisions at √sNN = 5.44 TeV. The data, corresponding to an integrated luminosity of 3.42 µb −1 , were collected in 2017 by the CMS experiment at the LHC. The yields are reported as functions of collision centrality and transverse momentum, pT, from 0.5 to 100 GeV. A previously reported pT spectrum from proton-proton collisions at √ s = 5.02 TeV is used for comparison after correcting for the difference in center-of-mass energy. The nuclear modification factors using this reference, R∗ AA, are constructed and compared to previous measurements and theoretical predictions. In head-on collisions, the R∗ AA has a value of 0.17 in the pT range of 6–8 GeV, but increases to approximately 0.7 at 100 GeV. Above ≈6 GeV, the XeXe data show a notably smaller suppression than previous results for lead-lead (PbPb) collisions at √sNN = 5.02 TeV when compared at the same centrality (i.e., the same fraction of total cross section). However, the XeXe suppression is slightly greater than that for PbPb in events having a similar number of participating nucleons.
format Article
author Sirunyan, A. M.
Tumasyan, A. R.
Adam, Wolfgang
Ambrogi, Federico
Asilar, Ece
Md. Ali, Mohd. Adli
author_facet Sirunyan, A. M.
Tumasyan, A. R.
Adam, Wolfgang
Ambrogi, Federico
Asilar, Ece
Md. Ali, Mohd. Adli
author_sort Sirunyan, A. M.
title Charged-particle nuclear modification factors in XeXe collisions at √sNN=5.44 TeV
title_short Charged-particle nuclear modification factors in XeXe collisions at √sNN=5.44 TeV
title_full Charged-particle nuclear modification factors in XeXe collisions at √sNN=5.44 TeV
title_fullStr Charged-particle nuclear modification factors in XeXe collisions at √sNN=5.44 TeV
title_full_unstemmed Charged-particle nuclear modification factors in XeXe collisions at √sNN=5.44 TeV
title_sort charged-particle nuclear modification factors in xexe collisions at √snn=5.44 tev
publisher Springer Verlag
publishDate 2018
url http://irep.iium.edu.my/70212/1/70212_Charged-particle%20nuclear%20modification%20factors%20in%20XeXe_article_new.pdf
http://irep.iium.edu.my/70212/2/70212_Charged-particle%20nuclear%20modification%20factors%20in%20XeXe_scopus.pdf
http://irep.iium.edu.my/70212/13/70212_Charged-particle%20nuclear%20modification%20factors_WOS.pdf
http://irep.iium.edu.my/70212/
https://link.springer.com/content/pdf/10.1007%2FJHEP10%282018%29138.pdf
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