Light (anti)nuclei production in Pb-Pb collisions at √sNN = 5.02 TeV

Detalhes bibliográficos
Autor(a) principal: Acharya, Shreyasi
Data de Publicação: 2023
Outros Autores: Gay Ducati, Maria Beatriz, Pereira, Luis Gustavo, ALICE Collaboration
Tipo de documento: Artigo
Idioma: eng
Título da fonte: Repositório Institucional da UFRGS
Texto Completo: http://hdl.handle.net/10183/268480
Resumo: The measurement of the production of deuterons, tritons and 3He and their antiparticles in Pb-Pb collisions at √sNN = 5.02 TeV is presented in this article. The measurements are carried out at midrapidity (|y| < 0.5) as a function of collision centrality using the ALICE detector. The pT-integrated yields, the coalescence parameters and the ratios to protons and antiprotons are reported and compared with nucleosynthesis models. The comparison of these results in different collision systems at different center-of-mass collision energies reveals a suppression of nucleus production in small systems. In the Statistical Hadronisation Model framework, this can be explained by a small correlation volume where the baryon number is conserved, as already shown in previous fluctuation analyses. However, a different size of the correlation volume is required to describe the proton yields in the same data sets. The coalescence model can describe this suppression by the fact that the wave functions of the nuclei are large and the fireball size starts to become comparable and even much smaller than the actual nucleus at low multiplicities.
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spelling Acharya, ShreyasiGay Ducati, Maria BeatrizPereira, Luis GustavoALICE Collaboration2023-12-16T03:26:09Z20230556-2813http://hdl.handle.net/10183/268480001186658The measurement of the production of deuterons, tritons and 3He and their antiparticles in Pb-Pb collisions at √sNN = 5.02 TeV is presented in this article. The measurements are carried out at midrapidity (|y| < 0.5) as a function of collision centrality using the ALICE detector. The pT-integrated yields, the coalescence parameters and the ratios to protons and antiprotons are reported and compared with nucleosynthesis models. The comparison of these results in different collision systems at different center-of-mass collision energies reveals a suppression of nucleus production in small systems. In the Statistical Hadronisation Model framework, this can be explained by a small correlation volume where the baryon number is conserved, as already shown in previous fluctuation analyses. However, a different size of the correlation volume is required to describe the proton yields in the same data sets. The coalescence model can describe this suppression by the fact that the wave functions of the nuclei are large and the fireball size starts to become comparable and even much smaller than the actual nucleus at low multiplicities.application/pdfengPhysical review. C, Nuclear physics. Melville. Vol. 107, no. 6 (June 2023), 064904, 16 p.Aceleradores de partículasColisao de ions pesadosLight (anti)nuclei production in Pb-Pb collisions at √sNN = 5.02 TeVEstrangeiroinfo:eu-repo/semantics/articleinfo:eu-repo/semantics/publishedVersioninfo:eu-repo/semantics/openAccessreponame:Repositório Institucional da UFRGSinstname:Universidade Federal do Rio Grande do Sul (UFRGS)instacron:UFRGSTEXT001186658.pdf.txt001186658.pdf.txtExtracted Texttext/plain85353http://www.lume.ufrgs.br/bitstream/10183/268480/2/001186658.pdf.txt97ebb4272b8f7f789fc9991742106ca4MD52ORIGINAL001186658.pdfTexto completo (inglês)application/pdf1722978http://www.lume.ufrgs.br/bitstream/10183/268480/1/001186658.pdffb492f4354a850dcbba8e96f53d77022MD5110183/2684802023-12-17 04:22:39.636618oai:www.lume.ufrgs.br:10183/268480Repositório de PublicaçõesPUBhttps://lume.ufrgs.br/oai/requestopendoar:2023-12-17T06:22:39Repositório Institucional da UFRGS - Universidade Federal do Rio Grande do Sul (UFRGS)false
dc.title.pt_BR.fl_str_mv Light (anti)nuclei production in Pb-Pb collisions at √sNN = 5.02 TeV
title Light (anti)nuclei production in Pb-Pb collisions at √sNN = 5.02 TeV
spellingShingle Light (anti)nuclei production in Pb-Pb collisions at √sNN = 5.02 TeV
Acharya, Shreyasi
Aceleradores de partículas
Colisao de ions pesados
title_short Light (anti)nuclei production in Pb-Pb collisions at √sNN = 5.02 TeV
title_full Light (anti)nuclei production in Pb-Pb collisions at √sNN = 5.02 TeV
title_fullStr Light (anti)nuclei production in Pb-Pb collisions at √sNN = 5.02 TeV
title_full_unstemmed Light (anti)nuclei production in Pb-Pb collisions at √sNN = 5.02 TeV
title_sort Light (anti)nuclei production in Pb-Pb collisions at √sNN = 5.02 TeV
author Acharya, Shreyasi
author_facet Acharya, Shreyasi
Gay Ducati, Maria Beatriz
Pereira, Luis Gustavo
ALICE Collaboration
author_role author
author2 Gay Ducati, Maria Beatriz
Pereira, Luis Gustavo
ALICE Collaboration
author2_role author
author
author
dc.contributor.author.fl_str_mv Acharya, Shreyasi
Gay Ducati, Maria Beatriz
Pereira, Luis Gustavo
ALICE Collaboration
dc.subject.por.fl_str_mv Aceleradores de partículas
Colisao de ions pesados
topic Aceleradores de partículas
Colisao de ions pesados
description The measurement of the production of deuterons, tritons and 3He and their antiparticles in Pb-Pb collisions at √sNN = 5.02 TeV is presented in this article. The measurements are carried out at midrapidity (|y| < 0.5) as a function of collision centrality using the ALICE detector. The pT-integrated yields, the coalescence parameters and the ratios to protons and antiprotons are reported and compared with nucleosynthesis models. The comparison of these results in different collision systems at different center-of-mass collision energies reveals a suppression of nucleus production in small systems. In the Statistical Hadronisation Model framework, this can be explained by a small correlation volume where the baryon number is conserved, as already shown in previous fluctuation analyses. However, a different size of the correlation volume is required to describe the proton yields in the same data sets. The coalescence model can describe this suppression by the fact that the wave functions of the nuclei are large and the fireball size starts to become comparable and even much smaller than the actual nucleus at low multiplicities.
publishDate 2023
dc.date.accessioned.fl_str_mv 2023-12-16T03:26:09Z
dc.date.issued.fl_str_mv 2023
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dc.identifier.issn.pt_BR.fl_str_mv 0556-2813
dc.identifier.nrb.pt_BR.fl_str_mv 001186658
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url http://hdl.handle.net/10183/268480
dc.language.iso.fl_str_mv eng
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dc.relation.ispartof.pt_BR.fl_str_mv Physical review. C, Nuclear physics. Melville. Vol. 107, no. 6 (June 2023), 064904, 16 p.
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