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$B_s$ and $B^+$ meson nuclear modification factors in PbPb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV with the CMS detector
Beauty quark production in heavy-ion collisions is considered to be one of the key measurements to address the flavour-dependence of in-medium energy loss in heavy-ion collisions. On the other hand, the measurement of the production of strange beauty mesons can provide fundamental insights into the...
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Lenguaje: | eng |
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2018
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Acceso en línea: | http://cds.cern.ch/record/2798192 |
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author | Falmagne, Guillaume |
author_facet | Falmagne, Guillaume |
author_sort | Falmagne, Guillaume |
collection | CERN |
description | Beauty quark production in heavy-ion collisions is considered to be one of the key measurements to address the flavour-dependence of in-medium energy loss in heavy-ion collisions. On the other hand, the measurement of the production of strange beauty mesons can provide fundamental insights into the relevance of mechanisms of beauty recombination in the quark-gluon plasma. In this talk, CMS will present the nuclear modification factor, $R_{AA}$, of fully reconstructed $B_{s}$ and $B^{+}$ mesons as a function of transverse momentum at $\sqrt{s_{NN}}=5.02$ = 5.02 TeV in PbPb collisions for the first time. The $R_{AA}$ double ratio between $B_{s}$ and $B^{+}$ is also presented. |
id | cern-2798192 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2018 |
record_format | invenio |
spelling | cern-27981922021-12-15T20:34:03Zhttp://cds.cern.ch/record/2798192engFalmagne, Guillaume$B_s$ and $B^+$ meson nuclear modification factors in PbPb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV with the CMS detectorDetectors and Experimental TechniquesBeauty quark production in heavy-ion collisions is considered to be one of the key measurements to address the flavour-dependence of in-medium energy loss in heavy-ion collisions. On the other hand, the measurement of the production of strange beauty mesons can provide fundamental insights into the relevance of mechanisms of beauty recombination in the quark-gluon plasma. In this talk, CMS will present the nuclear modification factor, $R_{AA}$, of fully reconstructed $B_{s}$ and $B^{+}$ mesons as a function of transverse momentum at $\sqrt{s_{NN}}=5.02$ = 5.02 TeV in PbPb collisions for the first time. The $R_{AA}$ double ratio between $B_{s}$ and $B^{+}$ is also presented.CMS-CR-2018-426oai:cds.cern.ch:27981922018-12-19 |
spellingShingle | Detectors and Experimental Techniques Falmagne, Guillaume $B_s$ and $B^+$ meson nuclear modification factors in PbPb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV with the CMS detector |
title | $B_s$ and $B^+$ meson nuclear modification factors in PbPb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV with the CMS detector |
title_full | $B_s$ and $B^+$ meson nuclear modification factors in PbPb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV with the CMS detector |
title_fullStr | $B_s$ and $B^+$ meson nuclear modification factors in PbPb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV with the CMS detector |
title_full_unstemmed | $B_s$ and $B^+$ meson nuclear modification factors in PbPb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV with the CMS detector |
title_short | $B_s$ and $B^+$ meson nuclear modification factors in PbPb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV with the CMS detector |
title_sort | $b_s$ and $b^+$ meson nuclear modification factors in pbpb collisions at $\sqrt{s_{nn}}$ = 5.02 tev with the cms detector |
topic | Detectors and Experimental Techniques |
url | http://cds.cern.ch/record/2798192 |
work_keys_str_mv | AT falmagneguillaume bsandbmesonnuclearmodificationfactorsinpbpbcollisionsatsqrtsnn502tevwiththecmsdetector |