cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.93887.v1/t11
title: "Figure 2.2" of "Longitudinal and azimuthal evolution of two-particle transverse momentum correlations in Pb-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 2.76 TeV"

description: Collision centrality evolution of the azimuthal widths of the two-particle transverse momentum correlations $G_{2}^{\rm CI}$ and $G_{2}^{\rm CD}$ in Pb--Pb collisions at $\sqrt{s_{\rm NN}}=2.76\;\text{TeV}$.
description: This paper presents the first measurements of the charge independent (CI) and charge dependent (CD) two-particle transverse momentum correlators $G_{2}^{\rm CI}$ and $G_{2}^{\rm CD}$ in Pb--Pb collisions at $\sqrt{s_{\text{NN}}} = 2.76\;\text{TeV}$ by the ALICE collaboration. The correlators are measured as a function of pair separation in pseudorapidity ($\Delta \eta$) and azimuth ($\Delta \varphi$) and as a function of collision centrality.The correlator $G_{2}^{\rm CI}$ exhibits a longitudinal broadening while undergoing a monotonic azimuthal narrowing from peripheral to central collisions. By contrast, $G_{2}^{\rm CD}$ exhibits a narrowing along both dimensions towards central events. These features are not reproduced by models such as HIJING and AMPT. However, the observed narrowing of the correlators is expected to result from the stronger transverse flow profiles produced in more central collisions and the longitudinal broadening is predicted to be sensitive to momentum currents and the shear viscosity per unit of entropy density $\eta/s$ of the matter produced in the collisions. The observed broadening is found to be consistent with the hypothesized lower bound of $\eta/s$ and is in qualitative agreement with values obtained from anisotropic flow measurements.
DOI: 10.17182/hepdata.93887.v1/t8
title: "Figure 1.8" of "Longitudinal and azimuthal evolution of two-particle transverse momentum correlations in Pb-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 2.76 TeV"

description: Azimuthal projection ($|\Delta\eta|&lt;1.6$) of the two-particle transverse momentum correlation $G_{2}^{\rm CI}$ for semi-central (30-40%) Pb--Pb collisions at $\sqrt{s_{\rm NN}}=2.76\;\text{TeV}$. Systematic uncertainty on the long-range mean correlator strength $\delta B = 3.8\times 10^{-3}$.
description: This paper presents the first measurements of the charge independent (CI) and charge dependent (CD) two-particle transverse momentum correlators $G_{2}^{\rm CI}$ and $G_{2}^{\rm CD}$ in Pb--Pb collisions at $\sqrt{s_{\text{NN}}} = 2.76\;\text{TeV}$ by the ALICE collaboration. The correlators are measured as a function of pair separation in pseudorapidity ($\Delta \eta$) and azimuth ($\Delta \varphi$) and as a function of collision centrality.The correlator $G_{2}^{\rm CI}$ exhibits a longitudinal broadening while undergoing a monotonic azimuthal narrowing from peripheral to central collisions. By contrast, $G_{2}^{\rm CD}$ exhibits a narrowing along both dimensions towards central events. These features are not reproduced by models such as HIJING and AMPT. However, the observed narrowing of the correlators is expected to result from the stronger transverse flow profiles produced in more central collisions and the longitudinal broadening is predicted to be sensitive to momentum currents and the shear viscosity per unit of entropy density $\eta/s$ of the matter produced in the collisions. The observed broadening is found to be consistent with the hypothesized lower bound of $\eta/s$ and is in qualitative agreement with values obtained from anisotropic flow measurements.
DOI: 10.15468/dl.h8j4q7
title: Occurrence Download

description: A dataset containing 1 species occurrences available in GBIF matching the query:
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 The dataset includes 1 records from 1 constituent datasets; see https://api.gbif.org/v1/occurrence/download/0003752-260120142942310/datasets/export for details.
 
Data from some individual datasets included in this download may be licensed under less restrictive terms.
DOI: 10.17182/hepdata.95539.v1/t1
title: "Table 1" of "Inclusive $\Upsilon$ production in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV"

description: $\Upsilon$(1S) differential cross section as a function of $y_{\rm cms}$, in p--Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV. The first uncertainty is statistical, while the second is the systematic.
description: CERN-LHC-ALICE. $\Upsilon$ production in $\mbox{p--Pb}$ interactions is studied at the centre-of-mass energy per nucleon--nucleon collision $\sqrt{s_{_{\rm {NN}}}} = 8.16$~TeV with the ALICE detector at the CERN LHC. The measurement is performed reconstructing bottomonium resonances via their dimuon decay channel, in the centre-of-mass rapidity intervals $2.03
DOI: 10.17182/hepdata.95539.v1/t2
title: "Table 2" of "Inclusive $\Upsilon$ production in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV"

description: $\Upsilon$(2S) differential cross section times as a function of $y_{\rm cms}$, in p--Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV. The first uncertainty is statistical, while the second is the systematic.
description: CERN-LHC-ALICE. $\Upsilon$ production in $\mbox{p--Pb}$ interactions is studied at the centre-of-mass energy per nucleon--nucleon collision $\sqrt{s_{_{\rm {NN}}}} = 8.16$~TeV with the ALICE detector at the CERN LHC. The measurement is performed reconstructing bottomonium resonances via their dimuon decay channel, in the centre-of-mass rapidity intervals $2.03
DOI: 10.17182/hepdata.95539.v1/t4
title: "Table 4" of "Inclusive $\Upsilon$ production in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV"

description: $\Upsilon$(1S) differential cross section as a function of $p_{\rm T}$, at forward rapidity at $\sqrt{s_{\rm NN}}$ = 8.16 TeV .The first uncertainty is statistical, while the second is the systematic.
description: CERN-LHC-ALICE. $\Upsilon$ production in $\mbox{p--Pb}$ interactions is studied at the centre-of-mass energy per nucleon--nucleon collision $\sqrt{s_{_{\rm {NN}}}} = 8.16$~TeV with the ALICE detector at the CERN LHC. The measurement is performed reconstructing bottomonium resonances via their dimuon decay channel, in the centre-of-mass rapidity intervals $2.03
DOI: 10.17182/hepdata.95539.v1/t6
title: "Table 6" of "Inclusive $\Upsilon$ production in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV"

description: Ratio of $\Upsilon$(2S) over $\Upsilon$(1S) yields in p--Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV .The first uncertainty is statistical, while the second is the systematic.
description: CERN-LHC-ALICE. $\Upsilon$ production in $\mbox{p--Pb}$ interactions is studied at the centre-of-mass energy per nucleon--nucleon collision $\sqrt{s_{_{\rm {NN}}}} = 8.16$~TeV with the ALICE detector at the CERN LHC. The measurement is performed reconstructing bottomonium resonances via their dimuon decay channel, in the centre-of-mass rapidity intervals $2.03
DOI: 10.17182/hepdata.95539.v1/t7
title: "Table 7" of "Inclusive $\Upsilon$ production in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV"

description: Ratio of $\Upsilon$(3S) over $\Upsilon$(1S) yields in p--Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV .The first uncertainty is statistical, while the second is the systematic.
description: CERN-LHC-ALICE. $\Upsilon$ production in $\mbox{p--Pb}$ interactions is studied at the centre-of-mass energy per nucleon--nucleon collision $\sqrt{s_{_{\rm {NN}}}} = 8.16$~TeV with the ALICE detector at the CERN LHC. The measurement is performed reconstructing bottomonium resonances via their dimuon decay channel, in the centre-of-mass rapidity intervals $2.03
DOI: 10.17182/hepdata.95539.v1/t8
title: "Table 8" of "Inclusive $\Upsilon$ production in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV"

description: $\Upsilon$(1S) $R_{\rm pPb}$ values at $\sqrt{s_{\rm NN}}$ = 8.16 TeV. The first uncertainty is statistical, the second is the uncorrelated systematic, while the third one is a correlated systematic uncertainty.
description: CERN-LHC-ALICE. $\Upsilon$ production in $\mbox{p--Pb}$ interactions is studied at the centre-of-mass energy per nucleon--nucleon collision $\sqrt{s_{_{\rm {NN}}}} = 8.16$~TeV with the ALICE detector at the CERN LHC. The measurement is performed reconstructing bottomonium resonances via their dimuon decay channel, in the centre-of-mass rapidity intervals $2.03
DOI: 10.17182/hepdata.95539.v1/t10
title: "Table 10" of "Inclusive $\Upsilon$ production in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV"

description: $\Upsilon$(1S) $R_{\rm pPb}$ as a function of $p_{\rm T}$ at backward rapidity at $\sqrt{s_{\rm NN}}$ = 8.16 TeV. The first uncertainty is statistical, the second is the uncorrelated systematic, while the third one is a correlated systematic uncertainty.
description: CERN-LHC-ALICE. $\Upsilon$ production in $\mbox{p--Pb}$ interactions is studied at the centre-of-mass energy per nucleon--nucleon collision $\sqrt{s_{_{\rm {NN}}}} = 8.16$~TeV with the ALICE detector at the CERN LHC. The measurement is performed reconstructing bottomonium resonances via their dimuon decay channel, in the centre-of-mass rapidity intervals $2.03
DOI: 10.17182/hepdata.95539.v1/t11
title: "Table 11" of "Inclusive $\Upsilon$ production in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV"

description: $\Upsilon$(1S) $R_{\rm pPb}$ as a function of $p_{\rm T}$ at forward rapidity at $\sqrt{s_{\rm NN}}$ = 8.16 TeV. The first uncertainty is statistical, the second is the uncorrelated systematic, while the third one is a correlated systematic uncertainty.
description: CERN-LHC-ALICE. $\Upsilon$ production in $\mbox{p--Pb}$ interactions is studied at the centre-of-mass energy per nucleon--nucleon collision $\sqrt{s_{_{\rm {NN}}}} = 8.16$~TeV with the ALICE detector at the CERN LHC. The measurement is performed reconstructing bottomonium resonances via their dimuon decay channel, in the centre-of-mass rapidity intervals $2.03
DOI: 10.17182/hepdata.95539.v1/t12
title: "Table 12" of "Inclusive $\Upsilon$ production in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV"

description: $\Upsilon$(1S) $Q_{\rm pPb}$ as a function of $$ at backward rapidity at $\sqrt{s_{\rm NN}}$ = 8.16 TeV. The first uncertainty is statistical, the second is the uncorrelated systematic, while the third one is a correlated systematic uncertainty.
description: CERN-LHC-ALICE. $\Upsilon$ production in $\mbox{p--Pb}$ interactions is studied at the centre-of-mass energy per nucleon--nucleon collision $\sqrt{s_{_{\rm {NN}}}} = 8.16$~TeV with the ALICE detector at the CERN LHC. The measurement is performed reconstructing bottomonium resonances via their dimuon decay channel, in the centre-of-mass rapidity intervals $2.03
DOI: 10.17182/hepdata.95539.v1/t13
title: "Table 13" of "Inclusive $\Upsilon$ production in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV"

description: $\Upsilon$(1S) $Q_{\rm pPb}$ as a function of $$ at forward rapidity at $\sqrt{s_{\rm NN}}$ = 8.16 TeV. The first uncertainty is statistical, the second is the uncorrelated systematic, while the third one is a correlated systematic uncertainty.
description: CERN-LHC-ALICE. $\Upsilon$ production in $\mbox{p--Pb}$ interactions is studied at the centre-of-mass energy per nucleon--nucleon collision $\sqrt{s_{_{\rm {NN}}}} = 8.16$~TeV with the ALICE detector at the CERN LHC. The measurement is performed reconstructing bottomonium resonances via their dimuon decay channel, in the centre-of-mass rapidity intervals $2.03
DOI: 10.17182/hepdata.95539.v1/t16
title: "Table 16" of "Inclusive $\Upsilon$ production in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV"

description: $\Upsilon$(3S) $R_{\rm pPb}$ values at $\sqrt{s_{\rm NN}}$ = 8.16 TeV. The first uncertainty is statistical, the second is the uncorrelated systematic, while the third one is a correlated systematic uncertainty.
description: CERN-LHC-ALICE. $\Upsilon$ production in $\mbox{p--Pb}$ interactions is studied at the centre-of-mass energy per nucleon--nucleon collision $\sqrt{s_{_{\rm {NN}}}} = 8.16$~TeV with the ALICE detector at the CERN LHC. The measurement is performed reconstructing bottomonium resonances via their dimuon decay channel, in the centre-of-mass rapidity intervals $2.03
DOI: 10.17182/hepdata.95539.v1/t3
title: "Table 3" of "Inclusive $\Upsilon$ production in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV"

description: $\Upsilon$(3S) differential cross section as a function of $y_{\rm cms}$, in p--Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV. The first uncertainty is statistical, while the second is the systematic.
description: CERN-LHC-ALICE. $\Upsilon$ production in $\mbox{p--Pb}$ interactions is studied at the centre-of-mass energy per nucleon--nucleon collision $\sqrt{s_{_{\rm {NN}}}} = 8.16$~TeV with the ALICE detector at the CERN LHC. The measurement is performed reconstructing bottomonium resonances via their dimuon decay channel, in the centre-of-mass rapidity intervals $2.03
DOI: 10.17182/hepdata.95539.v1/t5
title: "Table 5" of "Inclusive $\Upsilon$ production in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV"

description: $\Upsilon$(1S) differential cross section as a function of $p_{\rm T}$, at backward rapidity at $\sqrt{s_{\rm NN}}$ = 8.16 TeV .The first uncertainty is statistical, while the second is the systematic.
description: CERN-LHC-ALICE. $\Upsilon$ production in $\mbox{p--Pb}$ interactions is studied at the centre-of-mass energy per nucleon--nucleon collision $\sqrt{s_{_{\rm {NN}}}} = 8.16$~TeV with the ALICE detector at the CERN LHC. The measurement is performed reconstructing bottomonium resonances via their dimuon decay channel, in the centre-of-mass rapidity intervals $2.03
DOI: 10.17182/hepdata.95539.v1/t9
title: "Table 9" of "Inclusive $\Upsilon$ production in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV"

description: $\Upsilon$(1S) $R_{\rm pPb}$ as a function of $y_{\rm {cms}}$ at $\sqrt{s_{\rm NN}}$ = 8.16 TeV. The first uncertainty is statistical, the second is the uncorrelated systematic, while the third one is a correlated systematic uncertainty.
description: CERN-LHC-ALICE. $\Upsilon$ production in $\mbox{p--Pb}$ interactions is studied at the centre-of-mass energy per nucleon--nucleon collision $\sqrt{s_{_{\rm {NN}}}} = 8.16$~TeV with the ALICE detector at the CERN LHC. The measurement is performed reconstructing bottomonium resonances via their dimuon decay channel, in the centre-of-mass rapidity intervals $2.03
DOI: 10.17182/hepdata.94416.v1/t1
title: "Figure 4a" of "Production of (anti-)$^3$He and (anti-)$^3$H in p-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV"

description: Transverse momentum spectra of (anti-)$^3\mathrm{He}$ measured in $\mathrm{INEL}&gt;0$ p--Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$
description: No data abstract available.
DOI: 10.17182/hepdata.94416.v1/t2
title: "Figure 4b" of "Production of (anti-)$^3$He and (anti-)$^3$H in p-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV"

description: Transverse momentum spectra of (anti-)$^3\mathrm{H}$ measured in $\mathrm{INEL}&gt;0$ p--Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$
description: No data abstract available.
DOI: 10.17182/hepdata.95539.v1/t14
title: "Table 14" of "Inclusive $\Upsilon$ production in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV"

description: $\Upsilon$(1S) $R_{\rm pPb}$ values at $\sqrt{s_{\rm NN}}$ = 8.16 TeV. The first uncertainty is statistical, the second is the uncorrelated systematic, while the third one is a correlated systematic uncertainty.
description: CERN-LHC-ALICE. $\Upsilon$ production in $\mbox{p--Pb}$ interactions is studied at the centre-of-mass energy per nucleon--nucleon collision $\sqrt{s_{_{\rm {NN}}}} = 8.16$~TeV with the ALICE detector at the CERN LHC. The measurement is performed reconstructing bottomonium resonances via their dimuon decay channel, in the centre-of-mass rapidity intervals $2.03
DOI: 10.17182/hepdata.95539.v1/t15
title: "Table 15" of "Inclusive $\Upsilon$ production in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV"

description: $\Upsilon$(2S) $R_{\rm pPb}$ values at $\sqrt{s_{\rm NN}}$ = 8.16 TeV. The first uncertainty is statistical, the second is the uncorrelated systematic, while the third one is a correlated systematic uncertainty.
description: CERN-LHC-ALICE. $\Upsilon$ production in $\mbox{p--Pb}$ interactions is studied at the centre-of-mass energy per nucleon--nucleon collision $\sqrt{s_{_{\rm {NN}}}} = 8.16$~TeV with the ALICE detector at the CERN LHC. The measurement is performed reconstructing bottomonium resonances via their dimuon decay channel, in the centre-of-mass rapidity intervals $2.03
DOI: 10.17182/hepdata.95539.v1/t17
title: "Table 17" of "Inclusive $\Upsilon$ production in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV"

description: Ratio of $\Upsilon$(2S) to $\Upsilon$(1S) $R_{\rm pPb}$ at $\sqrt{s_{\rm NN}}$ = 8.16 TeV as a function of $y_{\rm cms}$ .The first uncertainty is statistical, while the second is the systematic.
description: CERN-LHC-ALICE. $\Upsilon$ production in $\mbox{p--Pb}$ interactions is studied at the centre-of-mass energy per nucleon--nucleon collision $\sqrt{s_{_{\rm {NN}}}} = 8.16$~TeV with the ALICE detector at the CERN LHC. The measurement is performed reconstructing bottomonium resonances via their dimuon decay channel, in the centre-of-mass rapidity intervals $2.03
DOI: 10.17182/hepdata.95539.v1/t18
title: "Table 18" of "Inclusive $\Upsilon$ production in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV"

description: Ratio of $\Upsilon$(3S) to $\Upsilon$(1S) $R_{\rm pPb}$ at $\sqrt{s_{\rm NN}}$ = 8.16 TeV as a function of $y_{\rm cms}$ .The first uncertainty is statistical, while the second is the systematic.
description: CERN-LHC-ALICE. $\Upsilon$ production in $\mbox{p--Pb}$ interactions is studied at the centre-of-mass energy per nucleon--nucleon collision $\sqrt{s_{_{\rm {NN}}}} = 8.16$~TeV with the ALICE detector at the CERN LHC. The measurement is performed reconstructing bottomonium resonances via their dimuon decay channel, in the centre-of-mass rapidity intervals $2.03
DOI: 10.17182/hepdata.94416.v1/t10
title: "Figure 6a" of "Production of (anti-)$^3$He and (anti-)$^3$H in p-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV"

description: Mean transverse momentum obtained from the average of $^3\mathrm{He}$ and $^3\overline{\mathrm{He}}$ as a function of the mean charged-particle multiplicity density in p--Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV
description: No data abstract available.
DOI: 10.17182/hepdata.94416.v1/t11
title: "Figure 7a" of "Production of (anti-)$^3$He and (anti-)$^3$H in p-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV"

description: $(^3\mathrm{He} +\,^3\overline{\mathrm{He}}) / (\mathrm{p} + \overline{\mathrm{p}})$ ratio in p$-$Pb as a function of the mean charged-particle multiplicity density
description: No data abstract available.
DOI: 10.17182/hepdata.94416.v1/t3
title: "Figure 4c" of "Production of (anti-)$^3$He and (anti-)$^3$H in p-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV"

description: $^3\overline{\mathrm{He}} /\,^3\mathrm{He}$ ratio in $\mathrm{INEL}&gt;0$ p--Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$
description: No data abstract available.
DOI: 10.17182/hepdata.94416.v1/t4
title: "Figure 4d" of "Production of (anti-)$^3$He and (anti-)$^3$H in p-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV"

description: $^3\overline{\mathrm{H}} /\,^3\mathrm{H}$ ratio in $\mathrm{INEL}&gt;0$ p--Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$
description: No data abstract available.
DOI: 10.17182/hepdata.94416.v1/t5
title: "Figure 5a" of "Production of (anti-)$^3$He and (anti-)$^3$H in p-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV"

description: Transverse momentum spectra obtained from the average of $^3\mathrm{He}$ and $^3\overline{\mathrm{He}}$ for $\mathrm{INEL}&gt;0$ events in p$-$Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$
description: No data abstract available.
DOI: 10.17182/hepdata.94416.v1/t6
title: "Figure 5b" of "Production of (anti-)$^3$He and (anti-)$^3$H in p-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV"

description: Transverse momentum spectra obtained from the average of $^3\mathrm{He}$ and $^3\overline{\mathrm{He}}$ for events in 0$-$10% multiplicity class in p$-$Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$
description: No data abstract available.
DOI: 10.17182/hepdata.94416.v1/t7
title: "Figure 5c" of "Production of (anti-)$^3$He and (anti-)$^3$H in p-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV"

description: Transverse momentum spectra obtained from the average of $^3\mathrm{He}$ and $^3\overline{\mathrm{He}}$ for events in 10$-$20% multiplicity class in p$-$Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$
description: No data abstract available.
DOI: 10.17182/hepdata.94416.v1/t8
title: "Figure 5d" of "Production of (anti-)$^3$He and (anti-)$^3$H in p-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV"

description: Transverse momentum spectra obtained from the average of $^3\mathrm{He}$ and $^3\overline{\mathrm{He}}$ for events in 20$-$40% multiplicity class in p--Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$
description: No data abstract available.
DOI: 10.17182/hepdata.94416.v1/t9
title: "Figure 5e" of "Production of (anti-)$^3$He and (anti-)$^3$H in p-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV"

description: Transverse momentum spectra obtained from the average of $^3\mathrm{He}$ and $^3\overline{\mathrm{He}}$ for events in 40$-$100% multiplicity class in p--Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$
description: No data abstract available.
DOI: 10.17182/hepdata.94416.v1/t12
title: "Figure 7b" of "Production of (anti-)$^3$He and (anti-)$^3$H in p-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV"

description: $(^3\mathrm{H} +\,^3\overline{\mathrm{H}}) / (\mathrm{p} + \overline{\mathrm{p}})$ ratio in p$-$Pb as a function of the mean charged-particle multiplicity density
description: No data abstract available.
DOI: 10.17182/hepdata.94416.v1/t13
title: "Figure 8a" of "Production of (anti-)$^3$He and (anti-)$^3$H in p-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV"

description: Coalescence parameter $B_3$ calculated using the average of $\mathrm{INEL}&gt;0$ $^3\mathrm{He}$ and $^3\overline{\mathrm{He}}$ yields
description: No data abstract available.
DOI: 10.17182/hepdata.94416.v1/t14
title: "Figure 8b" of "Production of (anti-)$^3$He and (anti-)$^3$H in p-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV"

description: Coalescence parameter $B_3$ calculated using the average of $\mathrm{INEL}&gt;0$ $^3\mathrm{H}$ and $^3\overline{\mathrm{H}}$ yields
description: No data abstract available.