{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.77995.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1511864"}},{"@id":"https://doi.org/10.1103/PhysRevC.95.064606","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ALICE Collaboration"},"creator":{"@type":"Organization","name":"ALICE Collaboration"},"datePublished":"2017","description":"The production of K$^{*0}$ and $\\phi$ mesons are measured with the ALICE detector in pp and Pb-Pb collisions at the centre-of-mass energy per nucleon pair, $\\sqrt{s_{\\rm NN}}$ = 2.76 TeV. The invariant yield of K$^{*0}$ and $\\phi$ for rapidity $|y|<0.5$ are presented as a function of transverse momentum ($p_{\\rm T}$). The K$^{*0}$ and $\\phi$ invariant yields are compared with model calculation for inelastic pp collisions. The $p_{\\rm T}$ dependent particle ratios such K$^{*0}$/K, K$^{*0}/\\pi$, $\\phi$/K, $\\phi/\\pi$, p/K$^{*0}$ and p/$\\phi$ in inelastic pp and Pb--Pb collisions are obtained. The nuclear modification factor $R_{\\rm AA}$ was computed using a proton-proton reference at $\\sqrt{s} = 2.76$ TeV.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.77995.v1/t1","@type":"Dataset","description":"Invariant yield of K$^{*0}$ meson normalized to the number of inelastic pp collisions at $\\sqrt{s}=2.76~{\\rm TeV}$.","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.77995.v1/t2","@type":"Dataset","description":"Invariant yield of $\\phi$ meson normalized to the number of inelastic pp collisions at $\\sqrt{s}=2.76~{\\rm TeV}$.","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.77995.v1/t3","@type":"Dataset","description":"Invariant yield of K$^{*0}$ meson for 0-5$\\%$ centrality in Pb-Pb collisions at $\\sqrt{s_{\\rm NN}}=2.76~{\\rm TeV}$.","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.77995.v1/t4","@type":"Dataset","description":"Invariant yield of K$^{*0}$ meson for 5-10$\\%$ centrality in Pb-Pb collisions at $\\sqrt{s_{\\rm NN}}=2.76~{\\rm TeV}$.","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.77995.v1/t5","@type":"Dataset","description":"Invariant yield of K$^{*0}$ meson for 10-20$\\%$ centrality in Pb-Pb collisions at $\\sqrt{s_{\\rm NN}}=2.76~{\\rm TeV}$.","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.77995.v1/t6","@type":"Dataset","description":"Invariant yield of K$^{*0}$ meson for 20-30$\\%$ centrality in Pb-Pb collisions at $\\sqrt{s_{\\rm NN}}=2.76~{\\rm TeV}$.","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.77995.v1/t7","@type":"Dataset","description":"Invariant yield of K$^{*0}$ meson for 30-40$\\%$ centrality in Pb-Pb collisions at $\\sqrt{s_{\\rm NN}}=2.76~{\\rm TeV}$.","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.77995.v1/t8","@type":"Dataset","description":"Invariant yield of K$^{*0}$ meson for 40-50$\\%$ centrality in Pb-Pb collisions at $\\sqrt{s_{\\rm NN}}=2.76~{\\rm TeV}$.","name":"Table 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12"},{"@id":"https://doi.org/10.17182/hepdata.77995.v1/t13","@type":"Dataset","description":"Invariant yield of $\\phi$ meson for 30-40$\\%$ centrality in Pb-Pb collisions at $\\sqrt{s_{\\rm NN}}=2.76~{\\rm TeV}$.","name":"Table 13"},{"@id":"https://doi.org/10.17182/hepdata.77995.v1/t14","@type":"Dataset","description":"Invariant yield of $\\phi$ meson for 40-50$\\%$ centrality in Pb-Pb collisions at $\\sqrt{s_{\\rm NN}}=2.76~{\\rm TeV}$.","name":"Table 14"},{"@id":"https://doi.org/10.17182/hepdata.77995.v1/t15","@type":"Dataset","description":"Invariant yield of $\\phi$ meson for 60-80$\\%$ centrality in Pb-Pb collisions at $\\sqrt{s_{\\rm NN}}=2.76~{\\rm TeV}$.","name":"Table 15"},{"@id":"https://doi.org/10.17182/hepdata.77995.v1/t16","@type":"Dataset","description":"K$^{*0}$/K ratio as a function of $p_{\\rm T}$ for 0-5$\\%$ centrality in Pb-Pb collisions at $\\sqrt{s_{\\rm NN}}=2.76~{\\rm TeV}$.","name":"Table 16"},{"@id":"https://doi.org/10.17182/hepdata.77995.v1/t17","@type":"Dataset","description":"K$^{*0}$/K ratio as a function of $p_{\\rm T}$ for inelastic (INEL) pp collisions at $\\sqrt{s}=2.76~{\\rm TeV}$.","name":"Table 17"},{"@id":"https://doi.org/10.17182/hepdata.77995.v1/t18","@type":"Dataset","description":"$\\phi$/K ratio as a function of $p_{\\rm T}$ for 0-5$\\%$ centrality in Pb-Pb collisions at $\\sqrt{s_{\\rm NN}}=2.76~{\\rm TeV}$.","name":"Table 18"},{"@id":"https://doi.org/10.17182/hepdata.77995.v1/t19","@type":"Dataset","description":"$\\phi$/K ratio as a function of $p_{\\rm T}$ for inelastic (INEL) pp collisions at $\\sqrt{s}=2.76~{\\rm TeV}$.","name":"Table 19"},{"@id":"https://doi.org/10.17182/hepdata.77995.v1/t20","@type":"Dataset","description":"K$^{*0}/\\pi$ ratio as a function of $p_{\\rm T}$ for 0-5$\\%$ centrality in Pb-Pb collisions at $\\sqrt{s_{\\rm NN}}=2.76~{\\rm TeV}$.","name":"Table 20"},{"@id":"https://doi.org/10.17182/hepdata.77995.v1/t21","@type":"Dataset","description":"K$^{*0}/\\pi$ ratio as a function of $p_{\\rm T}$ for inelastic (INEL) pp collisions at $\\sqrt{s}=2.76~{\\rm TeV}$.","name":"Table 21"},{"@id":"https://doi.org/10.17182/hepdata.77995.v1/t22","@type":"Dataset","description":"$\\phi$/$\\pi$ ratio as a function of $p_{\\rm T}$ for 0-5$\\%$ centrality in Pb-Pb collisions at $\\sqrt{s_{\\rm NN}}=2.76~{\\rm TeV}$","name":"Table 22"},{"@id":"https://doi.org/10.17182/hepdata.77995.v1/t23","@type":"Dataset","description":"$\\phi$/$\\pi$ ratio as a function of $p_{\\rm T}$ for inelastic (INEL) pp collisions at $\\sqrt{s}=2.76~{\\rm TeV}$.","name":"Table 23"},{"@id":"https://doi.org/10.17182/hepdata.77995.v1/t24","@type":"Dataset","description":"p/K$^{*0}$ ratio as a function of $p_{\\rm T}$ for 0-5$\\%$ centrality in Pb-Pb collisions at $\\sqrt{s_{\\rm NN}}=2.76~{\\rm TeV}$.","name":"Table 24"},{"@id":"https://doi.org/10.17182/hepdata.77995.v1/t25","@type":"Dataset","description":"p/K$^{*0}$ ratio as a function of $p_{\\rm T}$ for 60-80$\\%$ centrality in Pb-Pb collisions at $\\sqrt{s_{\\rm NN}}=2.76~{\\rm TeV}$.","name":"Table 25"},{"@id":"https://doi.org/10.17182/hepdata.77995.v1/t26","@type":"Dataset","description":"p/K$^{*0}$ ratio as a function of $p_{\\rm T}$ for inelastic (INEL) pp collisions at $\\sqrt{s}=2.76~{\\rm TeV}$.","name":"Table 26"},{"@id":"https://doi.org/10.17182/hepdata.77995.v1/t27","@type":"Dataset","description":"p/$\\phi$ ratio as a function of $p_{\\rm T}$ for 0-5$\\%$ centrality in Pb-Pb collisions at $\\sqrt{s_{\\rm NN}}=2.76~{\\rm TeV}$.","name":"Table 27"},{"@id":"https://doi.org/10.17182/hepdata.77995.v1/t28","@type":"Dataset","description":"p/$\\phi$ ratio as a function of $p_{\\rm T}$ for 60-80$\\%$ centrality in Pb-Pb collisions at $\\sqrt{s_{\\rm NN}}=2.76~{\\rm TeV}$.","name":"Table 28"},{"@id":"https://doi.org/10.17182/hepdata.77995.v1/t29","@type":"Dataset","description":"p/$\\phi$ ratio as a function of $p_{\\rm T}$ for inelastic (INEL) pp collisions at $\\sqrt{s}=2.76~{\\rm TeV}$.","name":"Table 29"},{"@id":"https://doi.org/10.17182/hepdata.77995.v1/t30","@type":"Dataset","description":"Nuclear modification factor of average $K^{*0}$ and $\\overline{K^{*0}}$ as a function of $p_{\\rm T}$ for 0-5$\\%$ centrality in Pb-Pb collisions...","name":"Table 30"},{"@id":"https://doi.org/10.17182/hepdata.77995.v1/t31","@type":"Dataset","description":"Nuclear modification factor of average $K^{*0}$ and $\\overline{K^{*0}}$ as a function of $p_{\\rm T}$ for 5-10$\\%$ in Pb-Pb collisions at...","name":"Table 31"},{"@id":"https://doi.org/10.17182/hepdata.77995.v1/t32","@type":"Dataset","description":"Nuclear modification factor of average $K^{*0}$ and $\\overline{K^{*0}}$ as a function of $p_{\\rm T}$ for 20-30$\\%$ centrality in Pb-Pb collisions...","name":"Table 32"},{"@id":"https://doi.org/10.17182/hepdata.77995.v1/t33","@type":"Dataset","description":"Nuclear modification factor of average $K^{*0}$ and $\\overline{K^{*0}}$ as a function of $p_{\\rm T}$ for 40-50$\\%$ centrality in Pb-Pb collisions...","name":"Table 33"},{"@id":"https://doi.org/10.17182/hepdata.77995.v1/t34","@type":"Dataset","description":"Nuclear modification factor of $\\phi$ as a function of $p_{\\rm T}$ for 0-5$\\%$ in Pb-Pb collisions at $\\sqrt{s_{\\rm NN}}=2.76~{\\rm TeV}$.","name":"Table 34"},{"@id":"https://doi.org/10.17182/hepdata.77995.v1/t35","@type":"Dataset","description":"Nuclear modification factor of $\\phi$ as a function of $p_{\\rm T}$ for 5-10$\\%$ in Pb-Pb collisions at $\\sqrt{s_{\\rm NN}}=2.76~{\\rm TeV}$.","name":"Table 35"},{"@id":"https://doi.org/10.17182/hepdata.77995.v1/t36","@type":"Dataset","description":"Nuclear modification factor of $\\phi$ as a function of $p_{\\rm T}$ for 20-30$\\%$ in Pb-Pb collisions at $\\sqrt{s_{\\rm NN}}=2.76~{\\rm TeV}$.","name":"Table 36"},{"@id":"https://doi.org/10.17182/hepdata.77995.v1/t37","@type":"Dataset","description":"Nuclear modification factor of $\\phi$ as a function of $p_{\\rm T}$ for 40-50$\\%$ in Pb-Pb collisions at $\\sqrt{s_{\\rm NN}}=2.76~{\\rm TeV}$.","name":"Table 37"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1511864?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/77995"}],"inLanguage":"en","name":"K$^{*}(892)^{0}$ and $\\phi(1020)$ meson production at high transverse momentum in pp and Pb-Pb collisions at $\\sqrt{s_\\mathrm{NN}}$ = 2.76 TeV","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1511864?version=1","version":1}