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dc.contributor.authorMoriggi, Lucas Sosterpt_BR
dc.contributor.authorPeccini, Guilherme Müllerpt_BR
dc.contributor.authorMachado, Magno Valério Trindadept_BR
dc.date.accessioned2021-06-25T04:24:32Zpt_BR
dc.date.issued2021pt_BR
dc.identifier.issn0556-2821pt_BR
dc.identifier.urihttp://hdl.handle.net/10183/222830pt_BR
dc.description.abstractThe transverse momentum spectra of hadrons are calculated from the unintegrated gluon distribution (UGD) within the kT-factorization framework at small x. Starting from pp collisions, the modification caused by the nuclear medium is incorporated in the UGD at high energies, which is related to the nuclear shadowing phenomenon. Moreover, we consider that particle production from minijet decay is not enough to explain the pT spectra in AA collisions due to collective phenomena that take place after the hard collision. The Boltzmann-Gibbs blast wave distribution is utilized in order to evaluate the distribution of particle production in equilibrium. Data from the ALICE Collaboration for PbPb collisions at √s=2.76 TeV are analyzed, and the nuclear modification factor for pion production is computed.en
dc.format.mimetypeapplication/pdfpt_BR
dc.language.isoengpt_BR
dc.relation.ispartofPhysical Review. D, Particles and fields. Woodbury. Vol. 103, no. 3 (Feb. 2021), 034025, 8 p.pt_BR
dc.rightsOpen Accessen
dc.subjectAceleradores de partículaspt_BR
dc.subjectColisao de ions pesadospt_BR
dc.subjectProducao de pionspt_BR
dc.titleRole of nuclear gluon distribution on particle production in heavy ion collisionspt_BR
dc.typeArtigo de periódicopt_BR
dc.identifier.nrb001125239pt_BR
dc.type.originEstrangeiropt_BR


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