{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.84285.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1672860"}},{"@id":"https://doi.org/10.1103/PhysRevC.99.064901","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ALICE Collaboration"},"creator":{"@type":"Organization","name":"ALICE Collaboration"},"datePublished":"2019","description":"The production of $\\rho^{0}$ mesons is 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 yields of $\\rho^{0}$ for rapidity $|y|<0.5$ are presented as a function of transverse momentum ($p_{\\rm T}$). The $p_{\\rm T}$-integrated and $p_{\\rm T}$-differential particle ratios $\\rho^{0}/\\pi$ are obtained in pp and Pb--Pb collisions. The nuclear modification factors $R_{\\rm AA}$ are computed using a proton-proton reference at $\\sqrt{s} = 2.76$ TeV.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.84285.v1/t1","@type":"Dataset","description":"Reconstructed mass of $\\rho^{0}$ meson in pp collisions at $\\sqrt{s}=2.76~{\\rm TeV}$.","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.84285.v1/t2","@type":"Dataset","description":"Reconstructed mass of $\\rho^{0}$ meson in 0-20$\\%$ central Pb-Pb collisions at $\\sqrt{s_{\\rm NN}}=2.76~{\\rm TeV}$.","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.84285.v1/t3","@type":"Dataset","description":"Reconstructed mass of $\\rho^{0}$ meson in 20-40$\\%$ central Pb-Pb collisions at $\\sqrt{s_{\\rm NN}}=2.76~{\\rm TeV}$.","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.84285.v1/t4","@type":"Dataset","description":"Reconstructed mass of $\\rho^{0}$ meson in 40-60$\\%$ central Pb-Pb collisions at $\\sqrt{s_{\\rm NN}}=2.76~{\\rm TeV}$.","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.84285.v1/t5","@type":"Dataset","description":"Reconstructed mass of $\\rho^{0}$ meson in 60-80$\\%$ central Pb-Pb collisions at $\\sqrt{s_{\\rm NN}}=2.76~{\\rm TeV}$.","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.84285.v1/t6","@type":"Dataset","description":"Yield of $\\rho^{0}$ meson normalized to the number of inelastic pp collisions at $\\sqrt{s}=2.76~{\\rm TeV}$.","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.84285.v1/t7","@type":"Dataset","description":"Yield of $\\rho^{0}$ meson in 0-20$\\%$ central Pb-Pb collisions at $\\sqrt{s_{\\rm NN}}=2.76~{\\rm TeV}$.","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.84285.v1/t8","@type":"Dataset","description":"Yield of $\\rho^{0}$ meson in 20-40$\\%$ central Pb-Pb collisions at $\\sqrt{s_{\\rm NN}}=2.76~{\\rm TeV}$.","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.84285.v1/t9","@type":"Dataset","description":"Yield of $\\rho^{0}$ meson in 40-60$\\%$ central Pb-Pb collisions at $\\sqrt{s_{\\rm NN}}=2.76~{\\rm TeV}$.","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.84285.v1/t10","@type":"Dataset","description":"Yield of $\\rho^{0}$ meson in 60-80$\\%$ central Pb-Pb collisions at $\\sqrt{s_{\\rm NN}}=2.76~{\\rm TeV}$.","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.84285.v1/t11","@type":"Dataset","description":"Ratio of integrated yields $2\\rho^{0}/(\\pi^{+}+\\pi^{-})$ as a function of $(dN_{ch}/d\\eta)^{1/3}$ in pp and 0-20$\\%$, 20-40$\\%$, 40-60$\\%$, 60-80$\\%$ central Pb-Pb collisions...","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.84285.v1/t12","@type":"Dataset","description":"Mean transverse momentum of $\\rho^{0}$ meson as a function of $(dN_{ch}/d\\eta)^{1/3}$ in pp and 0-20$\\%$, 20-40$\\%$, 40-60$\\%$, 60-80$\\%$ central Pb-Pb...","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.84285.v1/t13","@type":"Dataset","description":"Ratio $2\\rho^{0}/(\\pi^{+}+\\pi^{-})$ as a function of $p_{T}$ in pp collisions at $\\sqrt{s}=2.76~{\\rm TeV}$.","name":"Table 13"},{"@id":"https://doi.org/10.17182/hepdata.84285.v1/t14","@type":"Dataset","description":"Ratio $2\\rho^{0}/(\\pi^{+}+\\pi^{-})$ as a function of $p_{T}$ in 0-20$\\%$ central Pb-Pb collisions at $\\sqrt{s_{\\rm NN}}=2.76~{\\rm TeV}$.","name":"Table 14"},{"@id":"https://doi.org/10.17182/hepdata.84285.v1/t15","@type":"Dataset","description":"Ratio $2\\rho^{0}/(\\pi^{+}+\\pi^{-})$ as a function of $p_{T}$ in 60-80$\\%$ central Pb-Pb collisions at $\\sqrt{s_{\\rm NN}}=2.76~{\\rm TeV}$.","name":"Table 15"},{"@id":"https://doi.org/10.17182/hepdata.84285.v1/t16","@type":"Dataset","description":"$R_{AA}$ as a function of $p_{T}$ in 0-20$\\%$ central Pb-Pb collisions at $\\sqrt{s_{\\rm NN}}=2.76~{\\rm TeV}$.","name":"Table 16"},{"@id":"https://doi.org/10.17182/hepdata.84285.v1/t17","@type":"Dataset","description":"$R_{AA}$ as a function of $p_{T}$ in 20-40$\\%$ central Pb-Pb collisions at $\\sqrt{s_{\\rm NN}}=2.76~{\\rm TeV}$.","name":"Table 17"},{"@id":"https://doi.org/10.17182/hepdata.84285.v1/t18","@type":"Dataset","description":"$R_{AA}$ as a function of $p_{T}$ in 40-60$\\%$ central Pb-Pb collisions at $\\sqrt{s_{\\rm NN}}=2.76~{\\rm TeV}$.","name":"Table 18"},{"@id":"https://doi.org/10.17182/hepdata.84285.v1/t19","@type":"Dataset","description":"$R_{AA}$ as a function of $p_{T}$ in 60-80$\\%$ central Pb-Pb collisions at $\\sqrt{s_{\\rm NN}}=2.76~{\\rm TeV}$.","name":"Table 19"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1672860?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/84285"}],"inLanguage":"en","name":"Production of the $\\rho$(770)${^{0}}$ meson in pp and Pb-Pb collisions at $\\sqrt{s_{\\rm NN}}$ = 2.76 TeV","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1672860?version=1","version":1}