{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.72720.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1418181"}},{"@id":"https://doi.org/10.1140/epjc/s10052-016-4088-7","@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 K$^{*}$(892)$^{0}$ and $\\phi$(1020) mesons has been measured in p-Pb collisions at $\\sqrt{s_{\\mathrm{NN}}}$ = 5.02 TeV. K$^{*0}$ and $\\phi$ are reconstructed via their decay into charged hadrons with the ALICE detector in the rapidity range $-0.5 < y <0$. The transverse momentum spectra, measured as a function of the multiplicity, have p$_{\\mathrm{T}}$ range from 0 to 15 GeV/$c$ for K$^{*0}$ and from 0.3 to 21 GeV/$c$ for $\\phi$. Integrated yields, mean transverse momenta and particle ratios are reported and compared with results in pp collisions at $\\sqrt{s}$ = 7 TeV and Pb-Pb collisions at $\\sqrt{s_{\\mathrm{NN}}}$ = 2.76 TeV. In Pb-Pb and p-Pb collisions, K$^{*0}$ and $\\phi$ probe the hadronic phase of the system and contribute to the study of particle formation mechanisms by comparison with other identified hadrons. For this purpose, the mean transverse momenta and the differential proton-to-$\\phi$ ratio are discussed as a function of the multiplicity of the event. The short-lived K$^{*0}$ is measured to investigate re-scattering effects, believed to be related to the size of the system and to the lifetime of the hadronic phase.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.72720.v1/t1","@type":"Dataset","description":"Average charged particle pseudo-rapidity density, $\\langle\\mathrm{d}N_{\\rm ch}/\\mathrm{d}\\eta_{\\mathrm{lab}}\\rangle$, measured at mid-rapidity in visible cross section event classes and average number of...","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.72720.v1/t2","@type":"Dataset","description":"$p_{\\rm T}$-differential yield of (K$^{*0}$ + $\\overline{K^{*0}}$)/2 in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (NSD). Additional systematic error: +- 3.1%...","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.72720.v1/t3","@type":"Dataset","description":"$p_{\\rm T}$-differential yield of (K$^{*0}$ + $\\overline{K^{*0}}$)/2 in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (0-20% multiplicity class).","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.72720.v1/t4","@type":"Dataset","description":"$p_{\\rm T}$-differential yield of (K$^{*0}$ + $\\overline{K^{*0}}$)/2 in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (20-40% multiplicity class).","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.72720.v1/t5","@type":"Dataset","description":"$p_{\\rm T}$-differential yield of (K$^{*0}$ + $\\overline{K^{*0}}$)/2 in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (40-60% multiplicity class).","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.72720.v1/t6","@type":"Dataset","description":"$p_{\\rm T}$-differential yield of (K$^{*0}$ + $\\overline{K^{*0}}$)/2 in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (60-80% multiplicity class).","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.72720.v1/t7","@type":"Dataset","description":"$p_{\\rm T}$-differential yield of (K$^{*0}$ + $\\overline{K^{*0}}$)/2 in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (80-100multiplicity class).","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.72720.v1/t8","@type":"Dataset","description":"$p_{\\rm T}$-differential invariant yield of $phi$ in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (NSD). Additional systematic error: +- 3.1% (normalization).","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.72720.v1/t9","@type":"Dataset","description":"$p_{\\rm T}$-differential yield of $\\phi$ in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (0-5% multiplicity class).","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.72720.v1/t10","@type":"Dataset","description":"$p_{\\rm T}$-differential yield of $\\phi$ in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (5-10% multiplicity class).","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.72720.v1/t11","@type":"Dataset","description":"$p_{\\rm T}$-differential yield of $\\phi$ in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (10-20% multiplicity class).","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.72720.v1/t12","@type":"Dataset","description":"$p_{\\rm T}$-differential yield of $\\phi$ in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (20-40% multiplicity class).","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.72720.v1/t13","@type":"Dataset","description":"$p_{\\rm T}$-differential yield of $\\phi$ in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (40-60% multiplicity class).","name":"Table 13"},{"@id":"https://doi.org/10.17182/hepdata.72720.v1/t14","@type":"Dataset","description":"$p_{\\rm T}$-differential yield of $\\phi$ in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (60-80% multiplicity class).","name":"Table 14"},{"@id":"https://doi.org/10.17182/hepdata.72720.v1/t15","@type":"Dataset","description":"$p_{\\rm T}$-differential yield of $\\phi$ in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (80-100% multiplicity class).","name":"Table 15"},{"@id":"https://doi.org/10.17182/hepdata.72720.v1/t16","@type":"Dataset","description":"$p_{\\rm T}$-integrated yield d$N$/d$y$ of (K$^{*0}$ + $\\overline{K^{*0}}$)/2 in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV. Yields are normalised to the...","name":"Table 16"},{"@id":"https://doi.org/10.17182/hepdata.72720.v1/t17","@type":"Dataset","description":"Mean $p_{\\rm T}$ of (K$^{*0}$ + $\\overline{K^{*0}}$)/2 in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV for each V0A multiplicity event class.","name":"Table 17"},{"@id":"https://doi.org/10.17182/hepdata.72720.v1/t18","@type":"Dataset","description":"$p_{\\rm T}$-integrated yield d$N$/d$y$ of $phi$ in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV. Yields are normalised to the visible cross...","name":"Table 18"},{"@id":"https://doi.org/10.17182/hepdata.72720.v1/t19","@type":"Dataset","description":"Mean $p_{\\rm T}$ of $phi$ in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV for each V0A multiplicity event class.","name":"Table 19"},{"@id":"https://doi.org/10.17182/hepdata.72720.v1/t20","@type":"Dataset","description":"Mean $p_{\\rm T}$ as function of the mass for particles measured with the ALICE detector in INEL pp collisions at...","name":"Table 20"},{"@id":"https://doi.org/10.17182/hepdata.72720.v1/t21","@type":"Dataset","description":"Mean $p_{\\rm T}$ as function of the mass for particles measured with the ALICE detector in 0-20% p-Pb collisions at...","name":"Table 21"},{"@id":"https://doi.org/10.17182/hepdata.72720.v1/t22","@type":"Dataset","description":"Ratio of $p_{\\rm T}$-differential yields of (p + $\\bar{p}$) and $\\phi$ in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (0-5$\\%$ multiplicity...","name":"Table 22"},{"@id":"https://doi.org/10.17182/hepdata.72720.v1/t23","@type":"Dataset","description":"Ratio of $p_{\\rm T}$-differential yields of (p + $\\bar{p}$) and $\\phi$ in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (5-10% multiplicity...","name":"Table 23"},{"@id":"https://doi.org/10.17182/hepdata.72720.v1/t24","@type":"Dataset","description":"Ratio of $p_{\\rm T}$-differential yields of (p + $\\bar{p}$) and $\\phi$ in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (10-20% multiplicity...","name":"Table 24"},{"@id":"https://doi.org/10.17182/hepdata.72720.v1/t25","@type":"Dataset","description":"Ratio of $p_{\\rm T}$-differential yields of (p + $\\bar{p}$) and $\\phi$ in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (20-40% multiplicity...","name":"Table 25"},{"@id":"https://doi.org/10.17182/hepdata.72720.v1/t26","@type":"Dataset","description":"Ratio of $p_{\\rm T}$-differential yields of (p + $\\bar{p}$) and $\\phi$ in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (40-60% multiplicity...","name":"Table 26"},{"@id":"https://doi.org/10.17182/hepdata.72720.v1/t27","@type":"Dataset","description":"Ratio of $p_{\\rm T}$-differential yields of (p + $\\bar{p}$) and $\\phi$ in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (60-80% multiplicity...","name":"Table 27"},{"@id":"https://doi.org/10.17182/hepdata.72720.v1/t28","@type":"Dataset","description":"Ratio of $p_{\\rm T}$-differential yields of (p + $\\bar{p}$) and $\\phi$ in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (80-100% multiplicity...","name":"Table 28"},{"@id":"https://doi.org/10.17182/hepdata.72720.v1/t29","@type":"Dataset","description":"Ratio of $p_{\\rm T}$-integrated yields of $(K^{*0}+\\overline{K^{*0}})$ to long lived hadrons for different V0A multiplicity classes in p-Pb collisions with...","name":"Table 29"},{"@id":"https://doi.org/10.17182/hepdata.72720.v1/t30","@type":"Dataset","description":"Ratio of $p_{\\rm T}$-integrated yields of 2$\\phi$ to long lived hadrons for different V0A multiplicity classes in p-Pb collisions with...","name":"Table 30"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1418181?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/72720"}],"inLanguage":"en","name":"Production of K$^{*}$(892)$^{0}$ and $\\phi$(1020) in p-Pb collisions at $\\sqrt{s_{\\mathrm{NN}}}$ = 5.02 TeV","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1418181?version=1","version":1}