{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.94416.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1762356"}},{"@id":"https://doi.org/10.1103/PhysRevC.101.044906","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ALICE Collaboration"},"creator":{"@type":"Organization","name":"ALICE Collaboration"},"datePublished":"2020","description":"The transverse momentum ($p_{\\rm{T}}$) differential yields of (anti-)$^3$He and (anti-)$^3$H measured in p-Pb collisions at $\\sqrt{s_{\\rm{NN}}}$ = 5.02 TeV with ALICE at the Large Hadron Collider (LHC) are presented. The ratios of the $p_{\\rm{T}}$-integrated yields of (anti-)$^3$He and (anti-)$^3$H to the proton yields are reported, as well as the $p_{\\rm{T}}$ dependence of the coalescence parameters $B_3$ for (anti-)$^3$He and (anti-)$^3$H. For (anti-)$^3$He, the results obtained in four classes of the mean charged-particle multiplicity density are also discussed. These results are compared to predictions from a canonical statistical hadronization model and coalescence approaches. An upper limit on the total yield of $^4\\bar{\\mathrm{He}}$ is determined.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.94416.v1/t1","@type":"Dataset","description":"Transverse momentum spectra of (anti-)$^3\\mathrm{He}$ measured in $\\mathrm{INEL}>0$ p--Pb collisions at $\\sqrt{s_\\mathrm{NN}} = 5.02$","name":"Figure 4a"},{"@id":"https://doi.org/10.17182/hepdata.94416.v1/t2","@type":"Dataset","description":"Transverse momentum spectra of (anti-)$^3\\mathrm{H}$ measured in $\\mathrm{INEL}>0$ p--Pb collisions at $\\sqrt{s_\\mathrm{NN}} = 5.02$","name":"Figure 4b"},{"@id":"https://doi.org/10.17182/hepdata.94416.v1/t3","@type":"Dataset","description":"$^3\\overline{\\mathrm{He}} /\\,^3\\mathrm{He}$ ratio in $\\mathrm{INEL}>0$ p--Pb collisions at $\\sqrt{s_\\mathrm{NN}} = 5.02$","name":"Figure 4c"},{"@id":"https://doi.org/10.17182/hepdata.94416.v1/t4","@type":"Dataset","description":"$^3\\overline{\\mathrm{H}} /\\,^3\\mathrm{H}$ ratio in $\\mathrm{INEL}>0$ p--Pb collisions at $\\sqrt{s_\\mathrm{NN}} = 5.02$","name":"Figure 4d"},{"@id":"https://doi.org/10.17182/hepdata.94416.v1/t5","@type":"Dataset","description":"Transverse momentum spectra obtained from the average of $^3\\mathrm{He}$ and $^3\\overline{\\mathrm{He}}$ for $\\mathrm{INEL}>0$ events in p$-$Pb collisions at $\\sqrt{s_\\mathrm{NN}} =...","name":"Figure 5a"},{"@id":"https://doi.org/10.17182/hepdata.94416.v1/t6","@type":"Dataset","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...","name":"Figure 5b"},{"@id":"https://doi.org/10.17182/hepdata.94416.v1/t7","@type":"Dataset","description":"Transverse momentum spectra obtained from the average of $^3\\mathrm{He}$ and $^3\\overline{\\mathrm{He}}$ for events in 10$-$20% multiplicity class in p$-$Pb collisions...","name":"Figure 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\\overline{\\mathrm{p}})$ ratio in p$-$Pb as a function of the mean charged-particle multiplicity density","name":"Figure 7a"},{"@id":"https://doi.org/10.17182/hepdata.94416.v1/t12","@type":"Dataset","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","name":"Figure 7b"},{"@id":"https://doi.org/10.17182/hepdata.94416.v1/t13","@type":"Dataset","description":"Coalescence parameter $B_3$ calculated using the average of $\\mathrm{INEL}>0$ $^3\\mathrm{He}$ and $^3\\overline{\\mathrm{He}}$ yields","name":"Figure 8a"},{"@id":"https://doi.org/10.17182/hepdata.94416.v1/t14","@type":"Dataset","description":"Coalescence parameter $B_3$ calculated using the average of $\\mathrm{INEL}>0$ $^3\\mathrm{H}$ and $^3\\overline{\\mathrm{H}}$ yields","name":"Figure 8b"},{"@id":"https://doi.org/10.17182/hepdata.94416.v1/t15","@type":"Dataset","description":"Ratio of (anti-)$^3$H and (anti-)$^3$He yields","name":"Figure 8c"},{"@id":"https://doi.org/10.17182/hepdata.94416.v1/t16","@type":"Dataset","description":"Coalescence parameter $B_3$ calculated using the average of $^3\\mathrm{He}$ and $^3\\overline{\\mathrm{He}}$ for $\\mathrm{INEL}>0$ events in p$-$Pb collisions at $\\sqrt{s_\\mathrm{NN}} =...","name":"Figure 9a"},{"@id":"https://doi.org/10.17182/hepdata.94416.v1/t17","@type":"Dataset","description":"Coalescence parameter $B_3$ calculated using the average of $^3\\mathrm{He}$ and $^3\\overline{\\mathrm{He}}$ for events in 0$-$10% multiplicity class in p$-$Pb collisions...","name":"Figure 9b"},{"@id":"https://doi.org/10.17182/hepdata.94416.v1/t18","@type":"Dataset","description":"Coalescence parameter $B_3$ calculated using the average of $^3\\mathrm{He}$ and $^3\\overline{\\mathrm{He}}$ for events in 10$-$20% multiplicity class in p$-$Pb collisions...","name":"Figure 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$^4\\overline{\\mathrm{He}}$ at 90$\\%$ confidence level corrected for the spin degeneracy factor $(2J...","name":"Figure 12c"},{"@id":"https://doi.org/10.17182/hepdata.94416.v1/t23","@type":"Dataset","description":"Integrated production yield obtained from the average of $^3\\mathrm{He}$ and $^3\\overline{\\mathrm{He}}$ for the different multiplicity classes and $\\mathrm{INEL} > 0$...","name":"Integrated yields (anti-)$^3\\mathrm{He}$"},{"@id":"https://doi.org/10.17182/hepdata.94416.v1/t24","@type":"Dataset","description":"Integrated production yield obtained from the average of $^3\\mathrm{H}$ and $^3\\overline{\\mathrm{H}}$ for $\\mathrm{INEL} > 0$ p--Pb collisions at $\\sqrt{s_\\mathrm{NN}} =...","name":"Integrated yields 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