{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.150017.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/2692205"}},{"@id":"https://doi.org/10.1103/PhysRevC.109.044902","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ALICE Collaboration"},"creator":{"@type":"Organization","name":"ALICE Collaboration"},"datePublished":"2024","description":"The production of K$^*$(892)$^\\pm$ meson resonance is measured at midrapidity ($|y|<0.5$) in Pb-Pb collisions at $\\sqrt{s_{\\rm NN}}=5.02$ TeV using the ALICE detector at the LHC. The resonance is reconstructed via its hadronic decay channel K$^*$(892)$^\\pm \\rightarrow \\rm{K^0_S \\pi^\\pm}$. The transverse momentum distributions are obtained for various centrality intervals in the $p_{\\rm T}$ range of 0.4-16 GeV/$c$. The reported measurements of integrated yields, mean transverse momenta, and particle yield ratios are consistent with previous ALICE measurements for K$^*$(892)$^0$. The $p_{\\rm T}$-integrated yield ratio 2K$^*$(892)$^\\pm$/($\\rm{K^+ + K^-}$) in central Pb-Pb collisions shows a significant suppression (9.3$\\sigma$) relative to pp collisions. Thermal model calculations overpredict the particle yield ratio. Although both simulations consider the hadronic phase, only HRG-PCE accurately represents the measurements, whereas MUSIC+SMASH tends to overpredict them. These observations, along with the kinetic freeze-out temperatures extracted from the yields of light-flavored hadrons using the HRG-PCE model, indicate a finite hadronic phase lifetime, which increases towards central collisions. The $p_{\\rm T}$-differential yield ratios 2K$^*$(892)$^\\pm$/($\\rm{K^+ + K^-}$) and 2K$^*$(892)$^\\pm$/($\\rm{\\pi^+ + \\pi^-}$) are suppressed by up to a factor of five at $p_{\\rm T}<2$ GeV/$c$ in central Pb-Pb collisions compared to pp collisions at $\\sqrt{s} =$ 5.02 TeV. Both particle ratios and are qualitatively consistent with expectations for rescattering effects in the hadronic phase. The nuclear modification factor shows a smooth evolution with centrality and is below unity at $p_{\\rm T}>8$ GeV/$c$, consistent with measurements for other light-flavored hadrons. The smallest values are observed in most central collisions, indicating larger energy loss of partons traversing the dense medium.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.150017.v1/t1","@type":"Dataset","description":"$p_{\\rm T}$-distributions of $\\rm{K}^{*}$ (average of particle and anti-particle) meson measured in Pb-Pb collisions at \\sqrt{s_{NN}}$ = 5.02 TeV for...","name":"Table 1a"},{"@id":"https://doi.org/10.17182/hepdata.150017.v1/t2","@type":"Dataset","description":"$p_{\\rm T}$-distributions of $\\rm{K}^{*}$ (average of particle and anti-particle) meson measured in Pb-Pb collisions at \\sqrt{s_{NN}}$ = 5.02 TeV for...","name":"Table 1b"},{"@id":"https://doi.org/10.17182/hepdata.150017.v1/t3","@type":"Dataset","description":"$p_{\\rm T}$-distributions of $\\rm{K}^{*}$ (average of particle and anti-particle) meson measured in Pb-Pb collisions at \\sqrt{s_{NN}}$ = 5.02 TeV for...","name":"Table 1c"},{"@id":"https://doi.org/10.17182/hepdata.150017.v1/t4","@type":"Dataset","description":"$p_{\\rm T}$-distributions of $\\rm{K}^{*}$ (average of particle and anti-particle) meson measured in Pb-Pb collisions at \\sqrt{s_{NN}}$ = 5.02 TeV for...","name":"Table 1d"},{"@id":"https://doi.org/10.17182/hepdata.150017.v1/t5","@type":"Dataset","description":"$p_{\\rm T}$-distributions of $\\rm{K}^{*}$ (average of particle and anti-particle) meson measured in Pb-Pb collisions at \\sqrt{s_{NN}}$ = 5.02 TeV for...","name":"Table 1e"},{"@id":"https://doi.org/10.17182/hepdata.150017.v1/t6","@type":"Dataset","description":"$p_{\\rm T}$-integrated yield d$N$/d$y$ of K$^{*}$ (average of particle and anti-particle) meson measured in Pb-Pb collisions at $\\sqrt{s_{NN}}$ = 5.02...","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.150017.v1/t7","@type":"Dataset","description":"Mean $p_{\\rm T}$ of K$^{*}$ (average of particle and anti-particle) meson measured in Pb-Pb collisions at $\\sqrt{s_{NN}}$ = 5.02 TeV.","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.150017.v1/t8","@type":"Dataset","description":"$p_{\\rm T}$-integrated yield ratio of $\\rm{K}^{*}$ (average of particleand anti-particle) to K (average of particle and anti-particle) measured in Pb-Pb...","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.150017.v1/t9","@type":"Dataset","description":"$p_{\\rm T}$ differential ratio $(\\rm{K}^{*\\pm} + \\rm{K}^{*\\mp}) / (\\rm{K}^{+}+\\rm{K}^{-})$ measured in Pb-Pb collisions at $\\sqrt{s_{NN}}$ = 5.02 TeV for 0-10\\%...","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.150017.v1/t10","@type":"Dataset","description":"$p_{\\rm T}$ differential ratio $(\\rm{K}^{*\\pm} + \\rm{K}^{*\\mp}) / (\\rm{K}^{+}+\\rm{K}^{-})$ measured in Pb-Pb collisions at $\\sqrt{s_{NN}}$ = 5.02 TeV for 60-80\\%...","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.150017.v1/t11","@type":"Dataset","description":"$p_{\\rm T}$ differential ratio $(\\rm{K}^{*\\pm} + \\rm{K}^{*\\mp}) / (\\rm{pi}^{+}+\\rm{pi}^{-})$ measured in Pb-Pb collisions at $\\sqrt{s_{NN}}$ = 5.02 TeV for 0-10\\%...","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.150017.v1/t12","@type":"Dataset","description":"$p_{\\rm T}$ differential ratio $(\\rm{K}^{*\\pm} + \\rm{K}^{*\\mp}) / (\\rm{pi}^{+}+\\rm{pi}^{-})$ measured in Pb-Pb collisions at $\\sqrt{s_{NN}}$ = 5.02 TeV for 60-80\\%...","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.150017.v1/t13","@type":"Dataset","description":"$p_{T}$-dependent nuclear modification factor of $\\rm{K}^{*}$ (average of particle and anti-particle) meson measured in Pb-Pb collisions at $\\sqrt{s_{NN}}$ = 5.02...","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.150017.v1/t14","@type":"Dataset","description":"$p_{T}$-dependent nuclear modification factor of $\\rm{K}^{*}$ (average of particle and anti-particle) meson measured in Pb-Pb collisions at $\\sqrt{s_{NN}}$ = 5.02...","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.150017.v1/t15","@type":"Dataset","description":"$p_{T}$-dependent nuclear modification factor of $\\rm{K}^{*}$ (average of particle and anti-particle) meson measured in Pb-Pb collisions at $\\sqrt{s_{NN}}$ = 5.02...","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.150017.v1/t16","@type":"Dataset","description":"$p_{T}$-dependent nuclear modification factor of $\\rm{K}^{*}$ (average of particle and anti-particle) meson measured in Pb-Pb collisions at $\\sqrt{s_{NN}}$ = 5.02...","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.150017.v1/t17","@type":"Dataset","description":"$p_{T}$-dependent nuclear modification factor of $\\rm{K}^{*}$ (average of particle and anti-particle) meson measured in Pb-Pb collisions at $\\sqrt{s_{NN}}$ = 5.02...","name":"Table 13"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins2692205?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/150017"}],"inLanguage":"en","name":"K$^{*}$(892)$^{\\pm}$ resonance production in Pb$-$Pb collisions at $\\sqrt{s_{\\rm NN}}$ = 5.02 TeV","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins2692205?version=1","version":1}