{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.81951.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1625294"}},{"@id":"https://doi.org/10.1103/PhysRevC.97.024615","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ALICE Collaboration"},"creator":{"@type":"Organization","name":"ALICE Collaboration"},"datePublished":"2018","description":"CERN-LHC. Invariant differential yields of deuterons and antideuterons in pp collisions at $\\sqrt{s}$ = 0.9, 2.76 and 7 TeV and the yields of tritons, $^{3}$He nuclei and their antinuclei at $\\sqrt{s}$ = 7 TeV have been measured with the ALICE detector at the CERN Large Hadron Collider. The measurements cover a wide transverse momentum ($p_{\\text{T}}$) range in the rapidity interval $|y|<0.5$, extending both the energy and the $p_{\\text{T}}$ reach of previous measurements up to 3 GeV/$c$ for $A=2$ and 6 GeV/$c$ for $A=3$. The coalescence parameters of (anti)deuterons and $^{3}\\overline{\\text{He}}$ nuclei exhibit an increasing trend with $p_{\\text{T}}$ and are found to be compatible with measurements in pA collisions at low $p_{\\text{T}}$ and lower energies. The integrated yields decrease by a factor of about 1000 for each increase of the mass number with one (anti)nucleon. Furthermore, the deuteron-to-proton ratio is reported as a function of the average charged particle multiplicity at different center-of-mass energies.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.81951.v1/t1","@type":"Dataset","description":"Invariant differential yield of deuterons and antideuterons in inelastic pp collisions at $\\sqrt{s}$ = 0.9 TeV. The uncertainties of $_{-0.8}^{+2.2}$%...","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.81951.v1/t2","@type":"Dataset","description":"Invariant differential yield of deuterons and antideuterons in inelastic pp collisions at $\\sqrt{s}$ = 2.76 TeV. The uncertainties of $_{-2.8}^{+5.2}$%...","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.81951.v1/t3","@type":"Dataset","description":"Invariant differential yield of deuterons and antideuterons in inelastic pp collisions at $\\sqrt{s}$ = 7 TeV. The uncertainties of $_{-2.0}^{+5.0}$%...","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.81951.v1/t4","@type":"Dataset","description":"Invariant differential yields of tritons and antitritons in inelastic pp collisions at $\\sqrt{s}$ = 7 TeV. The uncertainties of $_{-2.0}^{+5.0}$%...","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.81951.v1/t5","@type":"Dataset","description":"Invariant differential yields of $^{3}$He and $^{3}\\overline{\\text{He}}$ nuclei in inelastic pp collisions at $\\sqrt{s}$ = 7 TeV. The uncertainties of...","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.81951.v1/t6","@type":"Dataset","description":"Coalescence parameter ($B_{2}$) of deuterons and antideuterons in inelastic pp collisions at $\\sqrt{s}$ = 0.9 TeV.","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.81951.v1/t7","@type":"Dataset","description":"Coalescence parameter ($B_{2}$) of deuterons and antideuterons in inelastic pp collisions at $\\sqrt{s}$ = 2.76 TeV.","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.81951.v1/t8","@type":"Dataset","description":"Coalescence parameter ($B_{2}$) of deuterons and antideuterons in inelastic pp collisions at $\\sqrt{s}$ = 7 TeV.","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.81951.v1/t9","@type":"Dataset","description":"Coalescence parameter ($B_{3}$) of tritons and antitritons in inelastic pp collisions at $\\sqrt{s}$ = 7 TeV.","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.81951.v1/t10","@type":"Dataset","description":"Coalescence parameter ($B_{3}$) of $^{3}$He and $^{3}\\overline{\\text{He}}$ nuclei in inelastic pp collisions at $\\sqrt{s}$ = 7 TeV.","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.81951.v1/t11","@type":"Dataset","description":"Integrated deuteron-to-proton (d/p) and antideuteron-to-antiproton ($\\overline{\\text{d}}/\\overline{\\text{p}}$) ratios in inelastic pp collisions as a function of the average charged particle multiplicity...","name":"Table 11"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1625294?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/81951"}],"inLanguage":"en","name":"Production of deuterons, tritons, $^{3}$He nuclei and their anti-nuclei in pp collisions at $\\mathbf{\\sqrt{{\\textit s}}}$ = 0.9, 2.76 and 7 TeV","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1625294?version=1","version":1}