cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.141376.v1/t61
title: "triton over he3 as a function of pT in 0-10%% centrality" of "Light (anti)nuclei production in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}=5.02$ TeV"

description: Triton over $^3$He ratio in Pb-Pb collisions as a function $p_{\mathrm{T}}$ in 0-10% 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/t62
title: "triton over he3 as a function of pT in 10-30%% centrality" of "Light (anti)nuclei production in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}=5.02$ TeV"

description: Triton over $^3$He ratio in Pb-Pb collisions as a function $p_{\mathrm{T}}$ in 10-30% 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/t63
title: "triton over he3 as a function of pT in 30-50%% centrality" of "Light (anti)nuclei production in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}=5.02$ TeV"

description: Triton over $^3$He ratio in Pb-Pb collisions as a function $p_{\mathrm{T}}$ in 30-50% 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/t64
title: "triton over he3 as a function of pT in 50-90%% centrality" of "Light (anti)nuclei production in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}=5.02$ TeV"

description: Triton over $^3$He ratio in Pb-Pb collisions as a function $p_{\mathrm{T}}$ in 50-90% 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/t65
title: "triton_over_he3" of "Light (anti)nuclei production in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}=5.02$ TeV"

description: Triton over He3 ratio in Pb-Pb collisions as a function of the charged particle multiplicity density at mid-rapidity
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/t66
title: "yield_deuteron" of "Light (anti)nuclei production in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}=5.02$ TeV"

description: pT-integrated yields of deuteron in Pb-Pb collisions as a function of the charged particle multiplicity density at mid-rapidity
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.j9zapk
title: Occurrence Download

description: A dataset listing the 467 species recorded in GBIF matching the query:
{
 "and" : [
 "Country is India",
 "IucnRedListCategory is NT",
 "License is one of (CC-BY 4.0, CC0 1.0)",
 "OccurrenceStatus is Present"
 ]
}

 The dataset's 467 records were derived from 298 constituent datasets; see https://api.gbif.org/v1/occurrence/download/0023435-251025141854904/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/t67
title: "yield_antideuteron" of "Light (anti)nuclei production in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}=5.02$ TeV"

description: pT-integrated yields of antideuteron in Pb-Pb collisions as a function of the charged particle multiplicity density at mid-rapidity
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/t68
title: "meanpT_deuteron" of "Light (anti)nuclei production in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}=5.02$ TeV"

description: meanpT of deuteron in Pb-Pb collisions as a function of the charged particle multiplicity density at mid-rapidity
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/t69
title: "meanpT_antideuteron" of "Light (anti)nuclei production in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}=5.02$ TeV"

description: meanpT of antideuteron in Pb-Pb collisions as a function of the charged particle multiplicity density at mid-rapidity
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/t70
title: "yield_He3" of "Light (anti)nuclei production in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}=5.02$ TeV"

description: pT-integrated yields of ${}^{3}$He in Pb-Pb collisions as a function of the charged particle multiplicity density at mid-rapidity
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/t71
title: "yield_antiHe3" of "Light (anti)nuclei production in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}=5.02$ TeV"

description: pT-integrated yields of anti${}^{3}$He in Pb-Pb collisions as a function of the charged particle multiplicity density at mid-rapidity
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/t72
title: "meanpT_He3" of "Light (anti)nuclei production in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}=5.02$ TeV"

description: meanpTs of ${}^{3}$He in Pb-Pb collisions as a function of the charged particle multiplicity density at mid-rapidity
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/t73
title: "meanpT_antiHe3" of "Light (anti)nuclei production in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}=5.02$ TeV"

description: meanpT of anti${}^{3}$He in Pb-Pb collisions as a function of the charged particle multiplicity density at mid-rapidity
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.132486.v1/t1
title: "Figure 1.1" of "General balance functions of identified charged hadron pairs of $(\pi,{\rm K},{\rm p})$ in Pb$-$Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV"

description: Balance function $B^{\pi\pi}$ measured in semicentral Pb--Pb collisions at $\sqrt{s_{\rm NN}}=2.76\;\text{TeV}$ ($\pi,{\rm K}: 0.2 \leq p_{\rm T} \leq 2.0\;{\rm GeV}/c$; ${\rm p}: 0.5 \leq p_{\rm T} \leq 2.5\;{\rm GeV}/c$).
description: First measurements of balance functions (BF) of all combinations of identified charged hadron $(\pi,\rm K,\rm p)$ pairs in Pb--Pb collisions at $\sqrt{s_{_{\rm NN}}} =$2.76 TeV recorded by the ALICE detector are presented. The BF measurements are carried out as two-dimensional differential correlators versus the relative rapidity ($\Delta y$) and azimuthal angle ($\Delta\varphi$) of hadron pairs, and studied as a function of collision centrality. The $\Delta\varphi$ dependence of BF is expected to be sensitive to the light quark diffusivity in the quark--gluon plasma. While the BF azimuthal widths of all pairs substantially decrease from peripheral to central collisions, the longitudinal widths exhibit mixed behaviors: BF of $\pi\pi$ and cross-species pairs narrow in more central collisions, whereas those of $\rm KK$ and $\rm pp$ are found to be independent of collision centrality. This dichotomy is qualitatively consistent with the presence of strong radial flow effects and the existence of two-stage quark production in relativistic heavy-ion collisions. Finally, the first measurements of the collision centrality evolution of BF integrals are presented, with the observation that relative charge balancing fractions are nearly independent of collision centrality in Pb--Pb collisions. Overall, the results presented provide new and challenging constraints for theoretical models of hadron production and transport in relativistic heavy-ion collisions.
DOI: 10.17182/hepdata.132486.v1/t2
title: "Figure 1.2" of "General balance functions of identified charged hadron pairs of $(\pi,{\rm K},{\rm p})$ in Pb$-$Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV"

description: Balance function $B^{{\rm KK}}$ measured in semicentral Pb--Pb collisions at $\sqrt{s_{\rm NN}}=2.76\;\text{TeV}$ ($\pi,{\rm K}: 0.2 \leq p_{\rm T} \leq 2.0\;{\rm GeV}/c$; ${\rm p}: 0.5 \leq p_{\rm T} \leq 2.5\;{\rm GeV}/c$).
description: First measurements of balance functions (BF) of all combinations of identified charged hadron $(\pi,\rm K,\rm p)$ pairs in Pb--Pb collisions at $\sqrt{s_{_{\rm NN}}} =$2.76 TeV recorded by the ALICE detector are presented. The BF measurements are carried out as two-dimensional differential correlators versus the relative rapidity ($\Delta y$) and azimuthal angle ($\Delta\varphi$) of hadron pairs, and studied as a function of collision centrality. The $\Delta\varphi$ dependence of BF is expected to be sensitive to the light quark diffusivity in the quark--gluon plasma. While the BF azimuthal widths of all pairs substantially decrease from peripheral to central collisions, the longitudinal widths exhibit mixed behaviors: BF of $\pi\pi$ and cross-species pairs narrow in more central collisions, whereas those of $\rm KK$ and $\rm pp$ are found to be independent of collision centrality. This dichotomy is qualitatively consistent with the presence of strong radial flow effects and the existence of two-stage quark production in relativistic heavy-ion collisions. Finally, the first measurements of the collision centrality evolution of BF integrals are presented, with the observation that relative charge balancing fractions are nearly independent of collision centrality in Pb--Pb collisions. Overall, the results presented provide new and challenging constraints for theoretical models of hadron production and transport in relativistic heavy-ion collisions.