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$B^0_s$ and $B^+$ nuclear modification factors in PbPb collisions at $\sqrt{s_\mathrm{NN}}$ = 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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Autor principal: Falmagne, Guillaume
Lenguaje:eng
Publicado: SISSA 2019
Materias:
Acceso en línea:https://dx.doi.org/10.22323/1.345.0143
http://cds.cern.ch/record/2684061
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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 results on the nuclear modification factor, $R_{AA}$, of fully reconstructed $\mathrm{B}_{s}$ and $\mathrm{B}^{+}$ mesons as a function of transverse momentum at $\sqrt{s_{NN}}=$ 5.02 TeV in PbPb collisions will be presented for the first time. The $R_{AA}$ double ratio between $\mathrm{B}^{0}_{s}$ and $\mathrm{B}^{+}$ will also be presented.
id oai-inspirehep.net-1731384
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2019
publisher SISSA
record_format invenio
spelling oai-inspirehep.net-17313842019-10-15T15:28:25Zdoi:10.22323/1.345.0143http://cds.cern.ch/record/2684061engFalmagne, Guillaume$B^0_s$ and $B^+$ nuclear modification factors in PbPb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV with the CMS detectorParticle Physics - ExperimentBeauty 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 results on the nuclear modification factor, $R_{AA}$, of fully reconstructed $\mathrm{B}_{s}$ and $\mathrm{B}^{+}$ mesons as a function of transverse momentum at $\sqrt{s_{NN}}=$ 5.02 TeV in PbPb collisions will be presented for the first time. The $R_{AA}$ double ratio between $\mathrm{B}^{0}_{s}$ and $\mathrm{B}^{+}$ will also be presented.SISSAoai:inspirehep.net:17313842019
spellingShingle Particle Physics - Experiment
Falmagne, Guillaume
$B^0_s$ and $B^+$ nuclear modification factors in PbPb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV with the CMS detector
title $B^0_s$ and $B^+$ nuclear modification factors in PbPb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV with the CMS detector
title_full $B^0_s$ and $B^+$ nuclear modification factors in PbPb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV with the CMS detector
title_fullStr $B^0_s$ and $B^+$ nuclear modification factors in PbPb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV with the CMS detector
title_full_unstemmed $B^0_s$ and $B^+$ nuclear modification factors in PbPb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV with the CMS detector
title_short $B^0_s$ and $B^+$ nuclear modification factors in PbPb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV with the CMS detector
title_sort $b^0_s$ and $b^+$ nuclear modification factors in pbpb collisions at $\sqrt{s_\mathrm{nn}}$ = 5.02 tev with the cms detector
topic Particle Physics - Experiment
url https://dx.doi.org/10.22323/1.345.0143
http://cds.cern.ch/record/2684061
work_keys_str_mv AT falmagneguillaume b0sandbnuclearmodificationfactorsinpbpbcollisionsatsqrtsmathrmnn502tevwiththecmsdetector