cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.128018.v1/t10
title: "Table 10" of "Measurement of inclusive charged-particle b-jet production in pp and p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV"

description: Fig. 14 left: The nuclear modification factor $R_{\mathrm{pPb}}$ of b jets as a function of $P_T$ from the IP method.
description: A measurement of the inclusive b-jet production cross section is presented in pp and p-Pb collisions at $\sqrt{s_{\mathrm{NN}}}~=0.5~$TeV, using data collected with the ALICE detector at the LHC. The jets were reconstructed in the central rapidity region $|\eta|&lt;0.5$ from charged particles using the anti-$k_{\rm T}$ algorithm with resolution parameter $R=0.4$. Identification of b jets exploits the long lifetime of b-hadrons, using the properties of secondary vertices and impact parameter distributions. The $p_\mathrm{T}$-differential inclusive production cross section of b jets, as well as the corresponding inclusive b-jet fraction, are reported for pp and p-Pb collisions in the jet transverse momentum range $10 \le p_\mathrm{T,ch\,jet} \le 100$ GeV/$c$, together with the nuclear modification factor, $R_{\rm pPb}^\text{b-jet}$. The analysis thus extends the lower $p_\mathrm{T}$ limit of b-jet measurements at the LHC. The nuclear modification factor is found to be consistent with unity, indicating that the production of b jets in p-Pb at $\sqrt{s_{\mathrm{NN}}}~=0.5~$TeV is not affected by cold nuclear matter effects within the current precision. The measurements are well reproduced by POWHEG NLO pQCD calculations with PYTHIA fragmentation.
DOI: 10.17182/hepdata.128018.v1/t11
title: "Table 11" of "Measurement of inclusive charged-particle b-jet production in pp and p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV"

description: Fig. 14 right: The combined nuclear modification factor $R_{\mathrm{pPb}}$ of b jets as a function of $P_T$.
description: A measurement of the inclusive b-jet production cross section is presented in pp and p-Pb collisions at $\sqrt{s_{\mathrm{NN}}}~=0.5~$TeV, using data collected with the ALICE detector at the LHC. The jets were reconstructed in the central rapidity region $|\eta|&lt;0.5$ from charged particles using the anti-$k_{\rm T}$ algorithm with resolution parameter $R=0.4$. Identification of b jets exploits the long lifetime of b-hadrons, using the properties of secondary vertices and impact parameter distributions. The $p_\mathrm{T}$-differential inclusive production cross section of b jets, as well as the corresponding inclusive b-jet fraction, are reported for pp and p-Pb collisions in the jet transverse momentum range $10 \le p_\mathrm{T,ch\,jet} \le 100$ GeV/$c$, together with the nuclear modification factor, $R_{\rm pPb}^\text{b-jet}$. The analysis thus extends the lower $p_\mathrm{T}$ limit of b-jet measurements at the LHC. The nuclear modification factor is found to be consistent with unity, indicating that the production of b jets in p-Pb at $\sqrt{s_{\mathrm{NN}}}~=0.5~$TeV is not affected by cold nuclear matter effects within the current precision. The measurements are well reproduced by POWHEG NLO pQCD calculations with PYTHIA fragmentation.
DOI: 10.17182/hepdata.128018.v1/t7
title: "Table 7" of "Measurement of inclusive charged-particle b-jet production in pp and p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV"

description: Fig. 13 left: The b-jet fraction in pp collisions at $\sqrt{s}~=~5.02$ TeV.
description: A measurement of the inclusive b-jet production cross section is presented in pp and p-Pb collisions at $\sqrt{s_{\mathrm{NN}}}~=0.5~$TeV, using data collected with the ALICE detector at the LHC. The jets were reconstructed in the central rapidity region $|\eta|&lt;0.5$ from charged particles using the anti-$k_{\rm T}$ algorithm with resolution parameter $R=0.4$. Identification of b jets exploits the long lifetime of b-hadrons, using the properties of secondary vertices and impact parameter distributions. The $p_\mathrm{T}$-differential inclusive production cross section of b jets, as well as the corresponding inclusive b-jet fraction, are reported for pp and p-Pb collisions in the jet transverse momentum range $10 \le p_\mathrm{T,ch\,jet} \le 100$ GeV/$c$, together with the nuclear modification factor, $R_{\rm pPb}^\text{b-jet}$. The analysis thus extends the lower $p_\mathrm{T}$ limit of b-jet measurements at the LHC. The nuclear modification factor is found to be consistent with unity, indicating that the production of b jets in p-Pb at $\sqrt{s_{\mathrm{NN}}}~=0.5~$TeV is not affected by cold nuclear matter effects within the current precision. The measurements are well reproduced by POWHEG NLO pQCD calculations with PYTHIA fragmentation.
DOI: 10.17182/hepdata.128018.v1/t8
title: "Table 8" of "Measurement of inclusive charged-particle b-jet production in pp and p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV"

description: Fig. 13 right: The b-jet fraction in p-Pb collisions at $\sqrt{s_{\mathrm{NN}}~=~5.02$ TeV.
description: A measurement of the inclusive b-jet production cross section is presented in pp and p-Pb collisions at $\sqrt{s_{\mathrm{NN}}}~=0.5~$TeV, using data collected with the ALICE detector at the LHC. The jets were reconstructed in the central rapidity region $|\eta|&lt;0.5$ from charged particles using the anti-$k_{\rm T}$ algorithm with resolution parameter $R=0.4$. Identification of b jets exploits the long lifetime of b-hadrons, using the properties of secondary vertices and impact parameter distributions. The $p_\mathrm{T}$-differential inclusive production cross section of b jets, as well as the corresponding inclusive b-jet fraction, are reported for pp and p-Pb collisions in the jet transverse momentum range $10 \le p_\mathrm{T,ch\,jet} \le 100$ GeV/$c$, together with the nuclear modification factor, $R_{\rm pPb}^\text{b-jet}$. The analysis thus extends the lower $p_\mathrm{T}$ limit of b-jet measurements at the LHC. The nuclear modification factor is found to be consistent with unity, indicating that the production of b jets in p-Pb at $\sqrt{s_{\mathrm{NN}}}~=0.5~$TeV is not affected by cold nuclear matter effects within the current precision. The measurements are well reproduced by POWHEG NLO pQCD calculations with PYTHIA fragmentation.
DOI: 10.17182/hepdata.128018.v1/t9
title: "Table 9" of "Measurement of inclusive charged-particle b-jet production in pp and p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV"

description: Fig. 14 left: The nuclear modification factor $R_{\mathrm{pPb}}$ of b jets as a function of $P_T$ from the SV method.
description: A measurement of the inclusive b-jet production cross section is presented in pp and p-Pb collisions at $\sqrt{s_{\mathrm{NN}}}~=0.5~$TeV, using data collected with the ALICE detector at the LHC. The jets were reconstructed in the central rapidity region $|\eta|&lt;0.5$ from charged particles using the anti-$k_{\rm T}$ algorithm with resolution parameter $R=0.4$. Identification of b jets exploits the long lifetime of b-hadrons, using the properties of secondary vertices and impact parameter distributions. The $p_\mathrm{T}$-differential inclusive production cross section of b jets, as well as the corresponding inclusive b-jet fraction, are reported for pp and p-Pb collisions in the jet transverse momentum range $10 \le p_\mathrm{T,ch\,jet} \le 100$ GeV/$c$, together with the nuclear modification factor, $R_{\rm pPb}^\text{b-jet}$. The analysis thus extends the lower $p_\mathrm{T}$ limit of b-jet measurements at the LHC. The nuclear modification factor is found to be consistent with unity, indicating that the production of b jets in p-Pb at $\sqrt{s_{\mathrm{NN}}}~=0.5~$TeV is not affected by cold nuclear matter effects within the current precision. The measurements are well reproduced by POWHEG NLO pQCD calculations with PYTHIA fragmentation.
DOI: 10.17182/hepdata.127980.v1/t5
title: "Table 5" of "Measurement of prompt $\rm{D_{s}^{+}}$-meson production and azimuthal anisotropy in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV"

description: $p_\mathrm{{T}}$-differential production ratios of prompt $\mathrm{D}_s^+/\mathrm{D}^0$ mesons in the 0-10% centrality class in Pb-Pb collisions at $\sqrt{{s_\mathrm{NN}}}=5.02~\mathrm{{TeV}}$ in the rapidity interval $|y|&lt;0.5$.
Branching ratio of $\mathrm{D_s^+\to \phi\pi^+\to K^-K^+\pi^+}$: 0.0224
Branching ratio of $\mathrm{D^0 \to K^-\pi^+}$: 0.0395
description: The production yield and angular anisotropy of prompt $\mathrm{D_s^+}$ mesons were measured as a function of transverse momentum ($p_\mathrm{T}$) in Pb-Pb collisions at a centre-of-mass energy per nucleon pair $\sqrt{s_\mathrm{NN}}=5.02~\mathrm{TeV}$ collected with the ALICE detector at the LHC. $\mathrm{D_s^+}$ mesons and their charge conjugates were reconstructed at midrapidity ($|y|&lt;0.5$) from their hadronic decay channel $\mathrm{D_s^+\to \phi\pi^+}$, with $\mathrm{\phi\to K^-K^+}$, in the transverse momentum intervals $210~\mathrm{GeV}/c$, the measured $\mathrm{D_s^+}$-meson nuclear modification factor $R_\mathrm{AA}$ is consistent with the one of non-strange D mesons within uncertainties, while at lower $p_\mathrm{T}$ a hint for a $\mathrm{D_s^+}$-meson $R_\mathrm{AA}$ larger than that of non-strange D mesons is seen. The enhanced production of $\mathrm{D_s^+}$ relative to non-strange D mesons is also studied by comparing the $p_\mathrm{T}$-dependent $\mathrm{D_s^+}/\mathrm{D^0}$ production yield ratios in Pb-Pb and in pp collisions. The $\mathrm{D_s^+}/\mathrm{D^0}$ ratio measured in Pb-Pb collisions is found to be on average higher than that in pp collisions in the transverse-momentum interval $2
DOI: 10.17182/hepdata.127980.v1/t6
title: "Table 6" of "Measurement of prompt $\rm{D_{s}^{+}}$-meson production and azimuthal anisotropy in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV"

description: $p_\mathrm{{T}}$-differential production ratios of prompt $\mathrm{D}_s^+/\mathrm{D}^0$ mesons in the 30-50% centrality class in Pb-Pb collisions at $\sqrt{{s_\mathrm{NN}}}=5.02~\mathrm{{TeV}}$ in the rapidity interval $|y|&lt;0.5$.
Branching ratio of $\mathrm{D_s^+\to \phi\pi^+\to K^-K^+\pi^+}$: 0.0224
Branching ratio of $\mathrm{D^0 \to K^-\pi^+}$: 0.0395
description: The production yield and angular anisotropy of prompt $\mathrm{D_s^+}$ mesons were measured as a function of transverse momentum ($p_\mathrm{T}$) in Pb-Pb collisions at a centre-of-mass energy per nucleon pair $\sqrt{s_\mathrm{NN}}=5.02~\mathrm{TeV}$ collected with the ALICE detector at the LHC. $\mathrm{D_s^+}$ mesons and their charge conjugates were reconstructed at midrapidity ($|y|&lt;0.5$) from their hadronic decay channel $\mathrm{D_s^+\to \phi\pi^+}$, with $\mathrm{\phi\to K^-K^+}$, in the transverse momentum intervals $210~\mathrm{GeV}/c$, the measured $\mathrm{D_s^+}$-meson nuclear modification factor $R_\mathrm{AA}$ is consistent with the one of non-strange D mesons within uncertainties, while at lower $p_\mathrm{T}$ a hint for a $\mathrm{D_s^+}$-meson $R_\mathrm{AA}$ larger than that of non-strange D mesons is seen. The enhanced production of $\mathrm{D_s^+}$ relative to non-strange D mesons is also studied by comparing the $p_\mathrm{T}$-dependent $\mathrm{D_s^+}/\mathrm{D^0}$ production yield ratios in Pb-Pb and in pp collisions. The $\mathrm{D_s^+}/\mathrm{D^0}$ ratio measured in Pb-Pb collisions is found to be on average higher than that in pp collisions in the transverse-momentum interval $2
DOI: 10.17182/hepdata.127980.v1/t7
title: "Table 7" of "Measurement of prompt $\rm{D_{s}^{+}}$-meson production and azimuthal anisotropy in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV"

description: $p_\mathrm{{T}}$-differential prompt $\mathrm{D}_s^+/\mathrm{D}^0$ ratios in Pb-Pb collisions in the 0-10% centrality class at $\sqrt{s_\mathrm{NN}}=5.02~\mathrm{TeV}$ divided by those in pp collisions at the same energy.
description: The production yield and angular anisotropy of prompt $\mathrm{D_s^+}$ mesons were measured as a function of transverse momentum ($p_\mathrm{T}$) in Pb-Pb collisions at a centre-of-mass energy per nucleon pair $\sqrt{s_\mathrm{NN}}=5.02~\mathrm{TeV}$ collected with the ALICE detector at the LHC. $\mathrm{D_s^+}$ mesons and their charge conjugates were reconstructed at midrapidity ($|y|&lt;0.5$) from their hadronic decay channel $\mathrm{D_s^+\to \phi\pi^+}$, with $\mathrm{\phi\to K^-K^+}$, in the transverse momentum intervals $210~\mathrm{GeV}/c$, the measured $\mathrm{D_s^+}$-meson nuclear modification factor $R_\mathrm{AA}$ is consistent with the one of non-strange D mesons within uncertainties, while at lower $p_\mathrm{T}$ a hint for a $\mathrm{D_s^+}$-meson $R_\mathrm{AA}$ larger than that of non-strange D mesons is seen. The enhanced production of $\mathrm{D_s^+}$ relative to non-strange D mesons is also studied by comparing the $p_\mathrm{T}$-dependent $\mathrm{D_s^+}/\mathrm{D^0}$ production yield ratios in Pb-Pb and in pp collisions. The $\mathrm{D_s^+}/\mathrm{D^0}$ ratio measured in Pb-Pb collisions is found to be on average higher than that in pp collisions in the transverse-momentum interval $2
DOI: 10.17182/hepdata.127980.v1/t8
title: "Table 8" of "Measurement of prompt $\rm{D_{s}^{+}}$-meson production and azimuthal anisotropy in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV"

description: $p_\mathrm{{T}}$-differential prompt $\mathrm{D}_s^+/\mathrm{D}^0$ ratios in Pb-Pb collisions in the 30-50% centrality class at $\sqrt{s_\mathrm{NN}}=5.02~\mathrm{TeV}$ divided by those in pp collisions at the same energy.
description: The production yield and angular anisotropy of prompt $\mathrm{D_s^+}$ mesons were measured as a function of transverse momentum ($p_\mathrm{T}$) in Pb-Pb collisions at a centre-of-mass energy per nucleon pair $\sqrt{s_\mathrm{NN}}=5.02~\mathrm{TeV}$ collected with the ALICE detector at the LHC. $\mathrm{D_s^+}$ mesons and their charge conjugates were reconstructed at midrapidity ($|y|&lt;0.5$) from their hadronic decay channel $\mathrm{D_s^+\to \phi\pi^+}$, with $\mathrm{\phi\to K^-K^+}$, in the transverse momentum intervals $210~\mathrm{GeV}/c$, the measured $\mathrm{D_s^+}$-meson nuclear modification factor $R_\mathrm{AA}$ is consistent with the one of non-strange D mesons within uncertainties, while at lower $p_\mathrm{T}$ a hint for a $\mathrm{D_s^+}$-meson $R_\mathrm{AA}$ larger than that of non-strange D mesons is seen. The enhanced production of $\mathrm{D_s^+}$ relative to non-strange D mesons is also studied by comparing the $p_\mathrm{T}$-dependent $\mathrm{D_s^+}/\mathrm{D^0}$ production yield ratios in Pb-Pb and in pp collisions. The $\mathrm{D_s^+}/\mathrm{D^0}$ ratio measured in Pb-Pb collisions is found to be on average higher than that in pp collisions in the transverse-momentum interval $2
DOI: 10.17182/hepdata.127980.v1/t9
title: "Table 9" of "Measurement of prompt $\rm{D_{s}^{+}}$-meson production and azimuthal anisotropy in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV"

description: $p_\mathrm{T}$-differential elliptic flow coefficient $v_2$ of prompt $\mathrm{D_s^+}$ mesons in the 30-50% centrality class in Pb-Pb collisions at $\sqrt{{s_\mathrm{NN}}}=5.02~\mathrm{{TeV}}$.
description: The production yield and angular anisotropy of prompt $\mathrm{D_s^+}$ mesons were measured as a function of transverse momentum ($p_\mathrm{T}$) in Pb-Pb collisions at a centre-of-mass energy per nucleon pair $\sqrt{s_\mathrm{NN}}=5.02~\mathrm{TeV}$ collected with the ALICE detector at the LHC. $\mathrm{D_s^+}$ mesons and their charge conjugates were reconstructed at midrapidity ($|y|&lt;0.5$) from their hadronic decay channel $\mathrm{D_s^+\to \phi\pi^+}$, with $\mathrm{\phi\to K^-K^+}$, in the transverse momentum intervals $210~\mathrm{GeV}/c$, the measured $\mathrm{D_s^+}$-meson nuclear modification factor $R_\mathrm{AA}$ is consistent with the one of non-strange D mesons within uncertainties, while at lower $p_\mathrm{T}$ a hint for a $\mathrm{D_s^+}$-meson $R_\mathrm{AA}$ larger than that of non-strange D mesons is seen. The enhanced production of $\mathrm{D_s^+}$ relative to non-strange D mesons is also studied by comparing the $p_\mathrm{T}$-dependent $\mathrm{D_s^+}/\mathrm{D^0}$ production yield ratios in Pb-Pb and in pp collisions. The $\mathrm{D_s^+}/\mathrm{D^0}$ ratio measured in Pb-Pb collisions is found to be on average higher than that in pp collisions in the transverse-momentum interval $2
DOI: 10.17182/hepdata.141376.v1/t1
title: "Deuteron 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: Deuteron 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.
DOI: 10.17182/hepdata.141376.v1/t2
title: "Antideuteron 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: Antideuteron 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.
DOI: 10.17182/hepdata.141376.v1/t3
title: "Deuteron spectrum in 5-10% V0M centrality class" of "Light (anti)nuclei production in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}=5.02$ TeV"

description: Deuteron spectrum in 5-10% 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/t4
title: "Antideuteron spectrum in 5-10% V0M centrality class" of "Light (anti)nuclei production in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}=5.02$ TeV"

description: Antideuteron spectrum in 5-10% 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/t5
title: "Deuteron 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: Deuteron 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.