Light (anti)nuclei production in Pb-Pb collisions at √sNN = 5.02 TeV
Autor(a) principal: | |
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Data de Publicação: | 2023 |
Outros Autores: | , , |
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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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 |
dc.type.driver.fl_str_mv |
Estrangeiro info:eu-repo/semantics/article |
dc.type.status.fl_str_mv |
info:eu-repo/semantics/publishedVersion |
format |
article |
status_str |
publishedVersion |
dc.identifier.uri.fl_str_mv |
http://hdl.handle.net/10183/268480 |
dc.identifier.issn.pt_BR.fl_str_mv |
0556-2813 |
dc.identifier.nrb.pt_BR.fl_str_mv |
001186658 |
identifier_str_mv |
0556-2813 001186658 |
url |
http://hdl.handle.net/10183/268480 |
dc.language.iso.fl_str_mv |
eng |
language |
eng |
dc.relation.ispartof.pt_BR.fl_str_mv |
Physical review. C, Nuclear physics. Melville. Vol. 107, no. 6 (June 2023), 064904, 16 p. |
dc.rights.driver.fl_str_mv |
info:eu-repo/semantics/openAccess |
eu_rights_str_mv |
openAccess |
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application/pdf |
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