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Nuclear modification of $\Upsilon$ states in pPb collisions at $\sqrt{s_\mathrm{NN}} = 5.02~\mathrm{TeV}$

Production cross sections of $\Upsilon(\mathrm{1S})$, $\Upsilon(\mathrm{2S})$, and $\Upsilon(\mathrm{3S})$ states decaying into $\mu^{+}\mu^{-}$ in proton-lead (pPb) collisions are reported using data collected by the CMS experiment at $\sqrt{s_\mathrm{NN}}=5.02~\mathrm{TeV}$. Nuclear modification f...

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Autor principal: CMS Collaboration
Publicado: 2019
Materias:
Acceso en línea:http://cds.cern.ch/record/2699566
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author CMS Collaboration
author_facet CMS Collaboration
author_sort CMS Collaboration
collection CERN
description Production cross sections of $\Upsilon(\mathrm{1S})$, $\Upsilon(\mathrm{2S})$, and $\Upsilon(\mathrm{3S})$ states decaying into $\mu^{+}\mu^{-}$ in proton-lead (pPb) collisions are reported using data collected by the CMS experiment at $\sqrt{s_\mathrm{NN}}=5.02~\mathrm{TeV}$. Nuclear modification factors $R_\mathrm{pPb}$ for all three $\Upsilon$ states are obtained using measured proton-proton (pp) cross sections at the same collision energy. All $\Upsilon$ states are found to be suppressed in pPb collisions compared to pp collisions. The $\Upsilon$ $R_\mathrm{pPb}$ show a sequential ordering, with $\Upsilon(\mathrm{1S})$ least suppressed and $\Upsilon(\mathrm{3S})$ most suppressed, indicating presence of final-state modification of $\Upsilon$ states in pPb collisions. When presented as a function of transverse momentum $p_\mathrm{T}$ and center-of-mass rapidity $y_\mathrm{CM}$, the $R_\mathrm{pPb}$ of individual $\Upsilon$ states are found to be consistent with constant values; although there is slight indication of higher separation of the suppression level of excited states for low-$p_\mathrm{T}$ $\Upsilon$ in the lead-going direction, where more nuclear matter is present. The final-state comover interaction model, which predicts sequential suppression of bottomonia in pPb, is found to be in better agreement with $R_\mathrm{pPb}$ versus $y_\mathrm{CM}$ than initial-state models. The nuclear modification observed in pPb collisions is less pronounced than the strong modification observed in lead-lead collisions, suggesting presence of additional quark gluon plasma effects in the latter. Forward-backward production ratios $R_\mathrm{FB}$ of $\Upsilon$ states are reported as functions of event activity variables, obtained from midrapidity as well as forward and backward rapidity regions. The $R_\mathrm{FB}$ for all $\Upsilon$ states are found to be consistent with unity and constant with increasing event activity, irrespective of the rapidity region used to measure activity.
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institution Organización Europea para la Investigación Nuclear
publishDate 2019
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spelling cern-26995662022-02-24T08:04:50Zhttp://cds.cern.ch/record/2699566CMS CollaborationNuclear modification of $\Upsilon$ states in pPb collisions at $\sqrt{s_\mathrm{NN}} = 5.02~\mathrm{TeV}$Nuclear Physics - ExperimentProduction cross sections of $\Upsilon(\mathrm{1S})$, $\Upsilon(\mathrm{2S})$, and $\Upsilon(\mathrm{3S})$ states decaying into $\mu^{+}\mu^{-}$ in proton-lead (pPb) collisions are reported using data collected by the CMS experiment at $\sqrt{s_\mathrm{NN}}=5.02~\mathrm{TeV}$. Nuclear modification factors $R_\mathrm{pPb}$ for all three $\Upsilon$ states are obtained using measured proton-proton (pp) cross sections at the same collision energy. All $\Upsilon$ states are found to be suppressed in pPb collisions compared to pp collisions. The $\Upsilon$ $R_\mathrm{pPb}$ show a sequential ordering, with $\Upsilon(\mathrm{1S})$ least suppressed and $\Upsilon(\mathrm{3S})$ most suppressed, indicating presence of final-state modification of $\Upsilon$ states in pPb collisions. When presented as a function of transverse momentum $p_\mathrm{T}$ and center-of-mass rapidity $y_\mathrm{CM}$, the $R_\mathrm{pPb}$ of individual $\Upsilon$ states are found to be consistent with constant values; although there is slight indication of higher separation of the suppression level of excited states for low-$p_\mathrm{T}$ $\Upsilon$ in the lead-going direction, where more nuclear matter is present. The final-state comover interaction model, which predicts sequential suppression of bottomonia in pPb, is found to be in better agreement with $R_\mathrm{pPb}$ versus $y_\mathrm{CM}$ than initial-state models. The nuclear modification observed in pPb collisions is less pronounced than the strong modification observed in lead-lead collisions, suggesting presence of additional quark gluon plasma effects in the latter. Forward-backward production ratios $R_\mathrm{FB}$ of $\Upsilon$ states are reported as functions of event activity variables, obtained from midrapidity as well as forward and backward rapidity regions. The $R_\mathrm{FB}$ for all $\Upsilon$ states are found to be consistent with unity and constant with increasing event activity, irrespective of the rapidity region used to measure activity.CMS-PAS-HIN-18-005oai:cds.cern.ch:26995662019
spellingShingle Nuclear Physics - Experiment
CMS Collaboration
Nuclear modification of $\Upsilon$ states in pPb collisions at $\sqrt{s_\mathrm{NN}} = 5.02~\mathrm{TeV}$
title Nuclear modification of $\Upsilon$ states in pPb collisions at $\sqrt{s_\mathrm{NN}} = 5.02~\mathrm{TeV}$
title_full Nuclear modification of $\Upsilon$ states in pPb collisions at $\sqrt{s_\mathrm{NN}} = 5.02~\mathrm{TeV}$
title_fullStr Nuclear modification of $\Upsilon$ states in pPb collisions at $\sqrt{s_\mathrm{NN}} = 5.02~\mathrm{TeV}$
title_full_unstemmed Nuclear modification of $\Upsilon$ states in pPb collisions at $\sqrt{s_\mathrm{NN}} = 5.02~\mathrm{TeV}$
title_short Nuclear modification of $\Upsilon$ states in pPb collisions at $\sqrt{s_\mathrm{NN}} = 5.02~\mathrm{TeV}$
title_sort nuclear modification of $\upsilon$ states in ppb collisions at $\sqrt{s_\mathrm{nn}} = 5.02~\mathrm{tev}$
topic Nuclear Physics - Experiment
url http://cds.cern.ch/record/2699566
work_keys_str_mv AT cmscollaboration nuclearmodificationofupsilonstatesinppbcollisionsatsqrtsmathrmnn502mathrmtev