cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.141376.v1/t6
title: "Antideuteron spectrum in 10-20% V0M centrality class" of "Light (anti)nuclei production in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}=5.02$ TeV"

description: Antideuteron spectrum in 10-20% V0M centrality class
description: The measurement of the production of deuterons, tritons and \ensuremath{^{3}\mathrm{He}}\xspace and their antiparticles in \mbox{Pb--Pb}\xspace collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV is presented in this article. The measurements are carried out at midrapidity ($|y| &lt; $ 0.5) as a function of collision centrality using the ALICE detector. The \ensuremath{p_{\rm T}}\xspace-integrated yields, the coalescence parameters and the ratios to protons are reported and compared with nucleosynthesis models. The comparison of these results in different collision systems at different centre-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.
DOI: 10.17182/hepdata.141376.v1/t7
title: "Deuteron spectrum in 20-30% V0M centrality class" of "Light (anti)nuclei production in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}=5.02$ TeV"

description: Deuteron spectrum in 20-30% V0M centrality class
description: The measurement of the production of deuterons, tritons and \ensuremath{^{3}\mathrm{He}}\xspace and their antiparticles in \mbox{Pb--Pb}\xspace collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV is presented in this article. The measurements are carried out at midrapidity ($|y| &lt; $ 0.5) as a function of collision centrality using the ALICE detector. The \ensuremath{p_{\rm T}}\xspace-integrated yields, the coalescence parameters and the ratios to protons are reported and compared with nucleosynthesis models. The comparison of these results in different collision systems at different centre-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.
DOI: 10.17182/hepdata.141376.v1/t8
title: "Antideuteron spectrum in 20-30% V0M centrality class" of "Light (anti)nuclei production in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}=5.02$ TeV"

description: Antideuteron spectrum in 20-30% V0M centrality class
description: The measurement of the production of deuterons, tritons and \ensuremath{^{3}\mathrm{He}}\xspace and their antiparticles in \mbox{Pb--Pb}\xspace collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV is presented in this article. The measurements are carried out at midrapidity ($|y| &lt; $ 0.5) as a function of collision centrality using the ALICE detector. The \ensuremath{p_{\rm T}}\xspace-integrated yields, the coalescence parameters and the ratios to protons are reported and compared with nucleosynthesis models. The comparison of these results in different collision systems at different centre-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.
DOI: 10.17182/hepdata.141376.v1/t9
title: "Deuteron spectrum in 30-40% V0M centrality class" of "Light (anti)nuclei production in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}=5.02$ TeV"

description: Deuteron spectrum in 30-40% V0M centrality class
description: The measurement of the production of deuterons, tritons and \ensuremath{^{3}\mathrm{He}}\xspace and their antiparticles in \mbox{Pb--Pb}\xspace collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV is presented in this article. The measurements are carried out at midrapidity ($|y| &lt; $ 0.5) as a function of collision centrality using the ALICE detector. The \ensuremath{p_{\rm T}}\xspace-integrated yields, the coalescence parameters and the ratios to protons are reported and compared with nucleosynthesis models. The comparison of these results in different collision systems at different centre-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.
DOI: 10.17182/hepdata.141376.v1/t10
title: "Antideuteron spectrum in 30-40% V0M centrality class" of "Light (anti)nuclei production in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}=5.02$ TeV"

description: Antideuteron spectrum in 30-40% V0M centrality class
description: The measurement of the production of deuterons, tritons and \ensuremath{^{3}\mathrm{He}}\xspace and their antiparticles in \mbox{Pb--Pb}\xspace collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV is presented in this article. The measurements are carried out at midrapidity ($|y| &lt; $ 0.5) as a function of collision centrality using the ALICE detector. The \ensuremath{p_{\rm T}}\xspace-integrated yields, the coalescence parameters and the ratios to protons are reported and compared with nucleosynthesis models. The comparison of these results in different collision systems at different centre-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.
DOI: 10.17182/hepdata.141376.v1/t11
title: "Deuteron spectrum in 40-50% V0M centrality class" of "Light (anti)nuclei production in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}=5.02$ TeV"

description: Deuteron spectrum in 40-50% V0M centrality class
description: The measurement of the production of deuterons, tritons and \ensuremath{^{3}\mathrm{He}}\xspace and their antiparticles in \mbox{Pb--Pb}\xspace collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV is presented in this article. The measurements are carried out at midrapidity ($|y| &lt; $ 0.5) as a function of collision centrality using the ALICE detector. The \ensuremath{p_{\rm T}}\xspace-integrated yields, the coalescence parameters and the ratios to protons are reported and compared with nucleosynthesis models. The comparison of these results in different collision systems at different centre-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.
DOI: 10.17182/hepdata.141376.v1/t12
title: "Antideuteron spectrum in 40-50% V0M centrality class" of "Light (anti)nuclei production in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}=5.02$ TeV"

description: Antideuteron spectrum in 40-50% V0M centrality class
description: The measurement of the production of deuterons, tritons and \ensuremath{^{3}\mathrm{He}}\xspace and their antiparticles in \mbox{Pb--Pb}\xspace collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV is presented in this article. The measurements are carried out at midrapidity ($|y| &lt; $ 0.5) as a function of collision centrality using the ALICE detector. The \ensuremath{p_{\rm T}}\xspace-integrated yields, the coalescence parameters and the ratios to protons are reported and compared with nucleosynthesis models. The comparison of these results in different collision systems at different centre-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.
DOI: 10.17182/hepdata.141376.v1/t13
title: "Deuteron spectrum in 50-60% V0M centrality class" of "Light (anti)nuclei production in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}=5.02$ TeV"

description: Deuteron spectrum in 50-60% V0M centrality class
description: The measurement of the production of deuterons, tritons and \ensuremath{^{3}\mathrm{He}}\xspace and their antiparticles in \mbox{Pb--Pb}\xspace collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV is presented in this article. The measurements are carried out at midrapidity ($|y| &lt; $ 0.5) as a function of collision centrality using the ALICE detector. The \ensuremath{p_{\rm T}}\xspace-integrated yields, the coalescence parameters and the ratios to protons are reported and compared with nucleosynthesis models. The comparison of these results in different collision systems at different centre-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.
DOI: 10.17182/hepdata.141376.v1/t14
title: "Antideuteron spectrum in 50-60% V0M centrality class" of "Light (anti)nuclei production in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}=5.02$ TeV"

description: Antideuteron spectrum in 50-60% V0M centrality class
description: The measurement of the production of deuterons, tritons and \ensuremath{^{3}\mathrm{He}}\xspace and their antiparticles in \mbox{Pb--Pb}\xspace collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV is presented in this article. The measurements are carried out at midrapidity ($|y| &lt; $ 0.5) as a function of collision centrality using the ALICE detector. The \ensuremath{p_{\rm T}}\xspace-integrated yields, the coalescence parameters and the ratios to protons are reported and compared with nucleosynthesis models. The comparison of these results in different collision systems at different centre-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.
DOI: 10.17182/hepdata.141376.v1/t15
title: "Deuteron spectrum in 60-70% V0M centrality class" of "Light (anti)nuclei production in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}=5.02$ TeV"

description: Deuteron spectrum in 60-70% V0M centrality class
description: The measurement of the production of deuterons, tritons and \ensuremath{^{3}\mathrm{He}}\xspace and their antiparticles in \mbox{Pb--Pb}\xspace collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV is presented in this article. The measurements are carried out at midrapidity ($|y| &lt; $ 0.5) as a function of collision centrality using the ALICE detector. The \ensuremath{p_{\rm T}}\xspace-integrated yields, the coalescence parameters and the ratios to protons are reported and compared with nucleosynthesis models. The comparison of these results in different collision systems at different centre-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.
DOI: 10.17182/hepdata.141376.v1/t16
title: "Antideuteron spectrum in 60-70% V0M centrality class" of "Light (anti)nuclei production in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}=5.02$ TeV"

description: Antideuteron spectrum in 60-70% V0M centrality class
description: The measurement of the production of deuterons, tritons and \ensuremath{^{3}\mathrm{He}}\xspace and their antiparticles in \mbox{Pb--Pb}\xspace collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV is presented in this article. The measurements are carried out at midrapidity ($|y| &lt; $ 0.5) as a function of collision centrality using the ALICE detector. The \ensuremath{p_{\rm T}}\xspace-integrated yields, the coalescence parameters and the ratios to protons are reported and compared with nucleosynthesis models. The comparison of these results in different collision systems at different centre-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.
DOI: 10.17182/hepdata.141376.v1/t17
title: "Deuteron spectrum in 70-80% V0M centrality class" of "Light (anti)nuclei production in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}=5.02$ TeV"

description: Deuteron spectrum in 70-80% V0M centrality class
description: The measurement of the production of deuterons, tritons and \ensuremath{^{3}\mathrm{He}}\xspace and their antiparticles in \mbox{Pb--Pb}\xspace collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV is presented in this article. The measurements are carried out at midrapidity ($|y| &lt; $ 0.5) as a function of collision centrality using the ALICE detector. The \ensuremath{p_{\rm T}}\xspace-integrated yields, the coalescence parameters and the ratios to protons are reported and compared with nucleosynthesis models. The comparison of these results in different collision systems at different centre-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.
DOI: 10.17182/hepdata.141376.v1/t18
title: "Antideuteron spectrum in 70-80% V0M centrality class" of "Light (anti)nuclei production in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}=5.02$ TeV"

description: Antideuteron spectrum in 70-80% V0M centrality class
description: The measurement of the production of deuterons, tritons and \ensuremath{^{3}\mathrm{He}}\xspace and their antiparticles in \mbox{Pb--Pb}\xspace collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV is presented in this article. The measurements are carried out at midrapidity ($|y| &lt; $ 0.5) as a function of collision centrality using the ALICE detector. The \ensuremath{p_{\rm T}}\xspace-integrated yields, the coalescence parameters and the ratios to protons are reported and compared with nucleosynthesis models. The comparison of these results in different collision systems at different centre-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.
DOI: 10.17182/hepdata.141376.v1/t19
title: "Deuteron spectrum in 80-90% V0M centrality class" of "Light (anti)nuclei production in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}=5.02$ TeV"

description: Deuteron spectrum in 80-90% V0M centrality class
description: The measurement of the production of deuterons, tritons and \ensuremath{^{3}\mathrm{He}}\xspace and their antiparticles in \mbox{Pb--Pb}\xspace collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV is presented in this article. The measurements are carried out at midrapidity ($|y| &lt; $ 0.5) as a function of collision centrality using the ALICE detector. The \ensuremath{p_{\rm T}}\xspace-integrated yields, the coalescence parameters and the ratios to protons are reported and compared with nucleosynthesis models. The comparison of these results in different collision systems at different centre-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.
DOI: 10.15468/dl.qdcw4t
title: Occurrence Download

description: A dataset listing the 8773 species recorded in GBIF matching the query:
{
 "and" : [
 "Country is India",
 "IucnRedListCategory is LC",
 "License is one of (CC-BY 4.0, CC0 1.0)",
 "OccurrenceStatus is Present"
 ]
}

 The dataset's 8773 records were derived from 774 constituent datasets; see https://api.gbif.org/v1/occurrence/download/0023437-251025141854904/datasets/export for details.
 
Data from some individual datasets included in this download may be licensed under less restrictive terms.
DOI: 10.17182/hepdata.141376.v1/t20
title: "Antideuteron spectrum in 80-90% V0M centrality class" of "Light (anti)nuclei production in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}=5.02$ TeV"

description: Antideuteron spectrum in 80-90% V0M centrality class
description: The measurement of the production of deuterons, tritons and \ensuremath{^{3}\mathrm{He}}\xspace and their antiparticles in \mbox{Pb--Pb}\xspace collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV is presented in this article. The measurements are carried out at midrapidity ($|y| &lt; $ 0.5) as a function of collision centrality using the ALICE detector. The \ensuremath{p_{\rm T}}\xspace-integrated yields, the coalescence parameters and the ratios to protons are reported and compared with nucleosynthesis models. The comparison of these results in different collision systems at different centre-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.
DOI: 10.17182/hepdata.141376.v1/t21
title: "He3 spectrum in 0-5% V0M centrality class" of "Light (anti)nuclei production in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}=5.02$ TeV"

description: $^3$He spectrum in 0-5% V0M centrality class
description: The measurement of the production of deuterons, tritons and \ensuremath{^{3}\mathrm{He}}\xspace and their antiparticles in \mbox{Pb--Pb}\xspace collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV is presented in this article. The measurements are carried out at midrapidity ($|y| &lt; $ 0.5) as a function of collision centrality using the ALICE detector. The \ensuremath{p_{\rm T}}\xspace-integrated yields, the coalescence parameters and the ratios to protons are reported and compared with nucleosynthesis models. The comparison of these results in different collision systems at different centre-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.