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Inclusive Psi(2S) production in p-Pb collisions with ALICE

The ALICE Collaboration has studied the inclusive $\psi(\rm 2S)$ production in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV at the CERN LHC. Measurements are performed, in the $\mu^{+}\mu^{-}$ decay channel, in a forward (2.03$<y_{\rm cms}<$3.53) and in a backward (-4.46$<y_{\rm cms}&l...

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Autor principal: Arnaldi, Roberta
Lenguaje:eng
Publicado: 2014
Materias:
Acceso en línea:https://dx.doi.org/10.1016/j.nuclphysa.2014.08.019
http://cds.cern.ch/record/1746614
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author Arnaldi, Roberta
author_facet Arnaldi, Roberta
author_sort Arnaldi, Roberta
collection CERN
description The ALICE Collaboration has studied the inclusive $\psi(\rm 2S)$ production in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV at the CERN LHC. Measurements are performed, in the $\mu^{+}\mu^{-}$ decay channel, in a forward (2.03$<y_{\rm cms}<$3.53) and in a backward (-4.46$<y_{\rm cms}<$-2.96) centre of mass rapidity ranges, as a function of transverse momentum or event activity. The $\psi(\rm 2S)$ production is compared to the $\rm J/\psi$ one through the double ratio $[\sigma_{\psi(\rm 2S)}/\sigma_{\rm J/\psi}]_{\rm pPb}/[\sigma_{\psi(\rm 2S)}/\sigma_{\rm J/\psi}]_{\rm pp}$ between the cross sections evaluated in p-Pb and pp collisions and by calculating the $\rm J/\psi$ and $\psi(\rm 2S)$ nuclear modification factors. Results indicate that the $\psi(\rm 2S)$ production is suppressed with respect to pp and, in particular in the backward rapidity region, the suppression is stronger than the $\rm J/\psi$ one. This unexpected difference between the $\rm J/\psi$ and $\psi(\rm 2S)$ behaviour, not accounted for by theoretical models based on nuclear parton shadowing and coherent energy loss mechanisms, indicates the presence of sizeable final state effects on the $\psi(\rm 2S)$ production.
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institution Organización Europea para la Investigación Nuclear
language eng
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spelling cern-17466142021-05-03T20:07:08Zdoi:10.1016/j.nuclphysa.2014.08.019http://cds.cern.ch/record/1746614engArnaldi, RobertaInclusive Psi(2S) production in p-Pb collisions with ALICEnucl-exThe ALICE Collaboration has studied the inclusive $\psi(\rm 2S)$ production in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV at the CERN LHC. Measurements are performed, in the $\mu^{+}\mu^{-}$ decay channel, in a forward (2.03$<y_{\rm cms}<$3.53) and in a backward (-4.46$<y_{\rm cms}<$-2.96) centre of mass rapidity ranges, as a function of transverse momentum or event activity. The $\psi(\rm 2S)$ production is compared to the $\rm J/\psi$ one through the double ratio $[\sigma_{\psi(\rm 2S)}/\sigma_{\rm J/\psi}]_{\rm pPb}/[\sigma_{\psi(\rm 2S)}/\sigma_{\rm J/\psi}]_{\rm pp}$ between the cross sections evaluated in p-Pb and pp collisions and by calculating the $\rm J/\psi$ and $\psi(\rm 2S)$ nuclear modification factors. Results indicate that the $\psi(\rm 2S)$ production is suppressed with respect to pp and, in particular in the backward rapidity region, the suppression is stronger than the $\rm J/\psi$ one. This unexpected difference between the $\rm J/\psi$ and $\psi(\rm 2S)$ behaviour, not accounted for by theoretical models based on nuclear parton shadowing and coherent energy loss mechanisms, indicates the presence of sizeable final state effects on the $\psi(\rm 2S)$ production.The ALICE Collaboration has studied the inclusive ψ(2S) production in p-Pb collisions at sNN=5.02 TeV at the CERN LHC. Measurements are performed, in the μ+μ− decay channel, in a forward (2.03 <ycms< 3.53) and in a backward (-4.46 <ycms< -2.96) centre of mass rapidity ranges, as a function of transverse momentum or event activity. The ψ(2S) production is compared to the J/ψ one through the double ratio [σψ(2S)/σJ/ψ]pPb/[σψ(2S)/σJ/ψ]pp between the cross sections evaluated in p-Pb and pp collisions and by calculating the J/ψ and ψ(2S) nuclear modification factors. Results indicate that the ψ(2S) production is suppressed with respect to pp and, in particular in the backward rapidity region, the suppression is stronger than the J/ψ one. This unexpected difference between the J/ψ and ψ(2S) behaviour, not accounted for by theoretical models based on nuclear parton shadowing and coherent energy loss mechanisms, indicates the presence of sizeable final state effects on the ψ(2S) production.The ALICE Collaboration has studied the inclusive $\psi(\rm 2S)$ production in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV at the CERN LHC. Measurements are performed, in the $\mu^{+}\mu^{-}$ decay channel, in a forward (2.03$<y_{\rm cms}<$3.53) and in a backward (-4.46$<y_{\rm cms}<$-2.96) centre of mass rapidity ranges, as a function of transverse momentum or event activity. The $\psi(\rm 2S)$ production is compared to the $\rm J/\psi$ one through the double ratio $[\sigma_{\psi(\rm 2S)}/\sigma_{\rm J/\psi}]_{\rm pPb}/[\sigma_{\psi(\rm 2S)}/\sigma_{\rm J/\psi}]_{\rm pp}$ between the cross sections evaluated in p-Pb and pp collisions and by calculating the $\rm J/\psi$ and $\psi(\rm 2S)$ nuclear modification factors. Results indicate that the $\psi(\rm 2S)$ production is suppressed with respect to pp and, in particular in the backward rapidity region, the suppression is stronger than the $\rm J/\psi$ one. This unexpected difference between the $\rm J/\psi$ and $\psi(\rm 2S)$ behaviour, not accounted for by theoretical models based on nuclear parton shadowing and coherent energy loss mechanisms, indicates the presence of sizeable final state effects on the $\psi(\rm 2S)$ production.The ALICE Collaboration has studied the inclusive ψ(2S) production in p–Pb collisions at sNN=5.02 TeV at the CERN LHC. Measurements are performed, in the μ+μ− decay channel, in a forward ( 2.03<ycms<3.53 ) and in a backward ( −4.46<ycms<−2.96 ) centre of mass rapidity ranges, as a function of transverse momentum or event activity. The ψ(2S) production is compared to the J/ψ one through the double ratio [σψ(2S)/σJ/ψ]pPb/[σψ(2S)/σJ/ψ]pp between the cross sections evaluated in p–Pb and pp collisions and by calculating the J/ψ and ψ(2S) nuclear modification factors. Results indicate that the ψ(2S) production is suppressed with respect to pp and, in particular in the backward rapidity region, the suppression is stronger than the J/ψ one. This unexpected difference between the J/ψ and ψ(2S) behaviour, not accounted for by theoretical models based on nuclear parton shadowing and coherent energy loss mechanisms, indicates the presence of sizeable final state effects on the ψ(2S) production.arXiv:1407.7451oai:cds.cern.ch:17466142014-07-28
spellingShingle nucl-ex
Arnaldi, Roberta
Inclusive Psi(2S) production in p-Pb collisions with ALICE
title Inclusive Psi(2S) production in p-Pb collisions with ALICE
title_full Inclusive Psi(2S) production in p-Pb collisions with ALICE
title_fullStr Inclusive Psi(2S) production in p-Pb collisions with ALICE
title_full_unstemmed Inclusive Psi(2S) production in p-Pb collisions with ALICE
title_short Inclusive Psi(2S) production in p-Pb collisions with ALICE
title_sort inclusive psi(2s) production in p-pb collisions with alice
topic nucl-ex
url https://dx.doi.org/10.1016/j.nuclphysa.2014.08.019
http://cds.cern.ch/record/1746614
work_keys_str_mv AT arnaldiroberta inclusivepsi2sproductioninppbcollisionswithalice