{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.73749.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1415274"}},{"@id":"https://doi.org/10.1016/j.physletb.2016.07.050","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ALICE Collaboration"},"creator":{"@type":"Organization","name":"ALICE Collaboration"},"datePublished":"2016","description":"CERN-LHC.  The production of charged pions, kaons and (anti)protons has been measured at mid-rapidity ($-0.5 < y < 0$) in p-Pb collisions at $\\sqrt{s_{\\rm NN}}=5.02$ TeV using the ALICE detector at the LHC. Exploiting particle identification capabilities at high transverse momentum ($p_{\\rm T}$), the previously published $p_{\\rm T}$ spectra have been extended to include measurements up to 20 GeV/$c$ for seven event multiplicity classes. The $p_{\\rm T}$ spectra for pp collisions at $\\sqrt{s}=7$ TeV, needed to interpolate a pp reference spectrum, have also been extended up to 20 GeV/$c$ to measure the nuclear modification factor ($R_{\\rm pPb}$) in non-single diffractive p-Pb collisions. At intermediate transverse momentum ($2 < p_{\\rm T} < 10$ GeV/$c$) the proton-to-pion ratio increases with multiplicity in p-Pb collisions, a similar effect is not present in the kaon-to-pion ratio. The $p_{\\rm T}$ dependent structure of such increase is qualitatively similar to those observed in pp and heavy-ion collisions. At high $p_{\\rm T}$ ($>10$ GeV/$c$), the particle ratios are consistent with those reported for pp and Pb-Pb collisions at the LHC energies. At intermediate $p_{\\rm T}$ the (anti)proton $R_{\\rm pPb}$ shows a Cronin-like enhancement, while pions and kaons show little or no nuclear modification. At high $p_{\\rm T}$ the charged pion, kaon and (anti)proton $R_{\\rm pPb}$ are consistent with unity within statistical and systematic uncertainties.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.73749.v1/t1","@type":"Dataset","description":"pT-differential invariant yield of charged pions in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV, measured for different V0A multiplicity classes. The...","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.73749.v1/t2","@type":"Dataset","description":"pT-differential invariant yield of charged pions in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV, measured for NSD events. The first uncertainty...","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.73749.v1/t3","@type":"Dataset","description":"pT-differential invariant yield of charged kaons in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV, measured for different V0A multiplicity classes. The...","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.73749.v1/t4","@type":"Dataset","description":"pT-differential invariant yield of charged kaons in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV, measured for NSD events. The first uncertainty...","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.73749.v1/t5","@type":"Dataset","description":"pT-differential invariant yield of protons+antiprotons in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV, measured for different V0A multiplicity classes. The first...","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.73749.v1/t6","@type":"Dataset","description":"pT-differential invariant yield of protons+antiprotons in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV, measured for NSD events. The first uncertainty is...","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.73749.v1/t7","@type":"Dataset","description":"pT-differential invariant yield of charged pions in INEL p-p collisions with centre-of-mass energies 5.02 TeV and 7.0 TeV. The first...","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.73749.v1/t8","@type":"Dataset","description":"pT-differential invariant yield of charged kaons in INEL p-p collisions with centre-of-mass energies 5.02 TeV and 7.0 TeV. The first...","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.73749.v1/t9","@type":"Dataset","description":"pT-differential invariant yield of protons+antiprotons in INEL p-p collisions with centre-of-mass energies 5.02 TeV and 7.0 TeV. The first uncertainty...","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.73749.v1/t10","@type":"Dataset","description":"The nuclear modification factor RPPB of charged pions, charged kaons and protons+antiprotons as a function of pT in NSD p-Pb...","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.73749.v1/t11","@type":"Dataset","description":"pT-dependent charged kaon to charged pion production ratios in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV, measured for different V0A multiplicity...","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.73749.v1/t12","@type":"Dataset","description":"pT-dependent proton+antiproton to charged pion production ratios in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV, measured for different V0A multiplicity classes....","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.73749.v1/t13","@type":"Dataset","description":"pT-integrated charged kaon to charged pion and proton+antiproton to charged pion production ratios as a function of average multiplicities in...","name":"Table 13"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1415274?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/73749"}],"inLanguage":"en","name":"Multiplicity dependence of charged pion, kaon, and (anti)proton production at large transverse momentum in p-Pb collisions at $\\mathbf{\\sqrt{{\\textit s}_{\\rm NN}}}$ = 5.02 TeV","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1415274?version=1","version":1}