{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.136309.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1946970"}}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ALICE Collaboration"},"creator":{"@type":"Organization","name":"ALICE Collaboration"},"datePublished":"2023","description":"The production of $\\mathrm{K}^{*}(\\mathrm{892})^{0}$ and $\\mathrm{\\phi(1020)}$ resonances has been measured in p-Pb collisions at $\\sqrt{s_{\\rm NN}}$ = 8.16 TeV using the ALICE detector. Resonances are reconstructed via their hadronic decay channels in the rapidity interval $-$0.5 $<$$y$$<$ 0 and the transverse momentum spectra are measured for various multiplicity classes up to $p_{\\rm T}$ = 20 GeV/$c$ for $\\mathrm{K}^{*}(\\mathrm{892})^{0}$ and $p_{\\rm T}$ = 16 GeV/$c$ for $\\mathrm{\\phi(1020)}$. The $p_{\\rm T}$ -integrated yields and mean transverse momenta are reported and compared with previous results in pp, p-Pb and Pb-Pb collisions. The $x_{\\mathrm{T}}$ scaling for $\\mathrm{K}^{*}(\\mathrm{892})^{0}$ and $\\mathrm{\\phi(1020)}$ resonance production is newly tested in p-Pb collisions and found to hold in the high-$p_{\\rm T}$ region at LHC energies. The nuclear modification factors ($R_{\\rm pPb}$) as a function of $p_{\\rm T}$ for $\\mathrm{K}^{*0}$ and $\\mathrm{\\phi}$ at $\\sqrt{s_{NN}}$ = 8.16 TeV are presented along with the new $R_{\\rm pPb}$ measurements of $\\mathrm{K}^{*0}$, $\\mathrm{\\phi}$ , $\\Xi$, and $\\Omega$ at $\\sqrt{s_{\\rm NN}}$ = 5.02 TeV. At intermediate $p_{\\rm T}$ (2-8 GeV/$c$), $R_{\\rm pPb}$ of $\\Xi$, $\\Omega$ show a Cronin-like enhancement, while $\\mathrm{K}^{*0}$ and $\\mathrm{\\phi}$ show no or little nuclear modification. At high $p_{\\rm T}$ ($>$ 8 GeV/$c$), the $R_{\\rm pPb}$ values of all hadrons are consistent with unity within uncertainties. The $R_{\\rm pPb}$ of $\\mathrm{K}^{*}(\\mathrm{892})^{0}$ and $\\mathrm{\\phi(1020)}$ at $\\sqrt{s_{\\rm NN}}$ = 8.16 and 5.02 TeV show no significant energy dependence.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.136309.v1/t1","@type":"Dataset","description":"$p_{\\mathrm T}$-differential yield of $\\frac{\\mathrm{K^{*0}} + \\overline{\\mathrm{K^{*0}}}}{2}$ in p-Pb collisions at $\\sqrt{s_{\\mathrm{NN}}}~=~$8.16 TeV (NSD).","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.136309.v1/t2","@type":"Dataset","description":"$p_{\\mathrm T}$-differential yield of $\\frac{\\mathrm{K^{*0}} + \\overline{\\mathrm{K^{*0}}}}{2}$ in p-Pb collisions at $\\sqrt{s_{\\mathrm{NN}}}~=~$8.16 TeV (Multiplicity class 0-5%).","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.136309.v1/t3","@type":"Dataset","description":"$p_{\\mathrm T}$-differential yield of $\\frac{\\mathrm{K^{*0}} + \\overline{\\mathrm{K^{*0}}}}{2}$ in p-Pb collisions at $\\sqrt{s_{\\mathrm{NN}}}~=~$8.16 TeV (Multiplicity class 5-10%).","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.136309.v1/t4","@type":"Dataset","description":"$p_{\\mathrm T}$-differential yield of $\\frac{\\mathrm{K^{*0}} + \\overline{\\mathrm{K^{*0}}}}{2}$ in p-Pb collisions at $\\sqrt{s_{\\mathrm{NN}}}~=~$8.16 TeV (Multiplicity class 10-20%).","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.136309.v1/t5","@type":"Dataset","description":"$p_{\\mathrm T}$-differential yield of $\\frac{\\mathrm{K^{*0}} + \\overline{\\mathrm{K^{*0}}}}{2}$ in p-Pb collisions at $\\sqrt{s_{\\mathrm{NN}}}~=~$8.16 TeV (Multiplicity class 20-40%).","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.136309.v1/t6","@type":"Dataset","description":"$p_{\\mathrm T}$-differential yield of $\\frac{\\mathrm{K^{*0}} + \\overline{\\mathrm{K^{*0}}}}{2}$ in p-Pb collisions at $\\sqrt{s_{\\mathrm{NN}}}~=~$8.16 TeV (Multiplicity class 40-60%).","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.136309.v1/t7","@type":"Dataset","description":"$p_{\\mathrm T}$-differential yield of $\\frac{\\mathrm{K^{*0}} + \\overline{\\mathrm{K^{*0}}}}{2}$ in p-Pb collisions at $\\sqrt{s_{\\mathrm{NN}}}~=~$8.16 TeV (Multiplicity class 60-80%).","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.136309.v1/t8","@type":"Dataset","description":"$p_{\\mathrm T}$-differential yield of $\\frac{\\mathrm{K^{*0}} + \\overline{\\mathrm{K^{*0}}}}{2}$ in p-Pb collisions at $\\sqrt{s_{\\mathrm{NN}}}~=~$8.16 TeV (Multiplicity class 80-100%).","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.136309.v1/t9","@type":"Dataset","description":"$p_{\\mathrm T}$-differential yield of $\\phi$ in p-Pb collisions at $\\sqrt{s_{\\mathrm{NN}}}~=~$8.16 TeV (NSD).","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.136309.v1/t10","@type":"Dataset","description":"$p_{\\mathrm T}$-differential yield of $\\phi$ in p-Pb collisions at $\\sqrt{s_{\\mathrm{NN}}}~=~$8.16 TeV (Multiplicity class 0-5%).","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.136309.v1/t11","@type":"Dataset","description":"$p_{\\mathrm T}$-differential yield of $\\phi$ in p-Pb collisions at $\\sqrt{s_{\\mathrm{NN}}}~=~$8.16 TeV (Multiplicity class 5-10%).","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.136309.v1/t12","@type":"Dataset","description":"$p_{\\mathrm T}$-differential yield of $\\phi$ in p-Pb collisions at $\\sqrt{s_{\\mathrm{NN}}}~=~$8.16 TeV (Multiplicity class 10-20%).","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.136309.v1/t13","@type":"Dataset","description":"$p_{\\mathrm T}$-differential yield of $\\phi$ in p-Pb collisions at $\\sqrt{s_{\\mathrm{NN}}}~=~$8.16 TeV (Multiplicity class 20-40%).","name":"Table 13"},{"@id":"https://doi.org/10.17182/hepdata.136309.v1/t14","@type":"Dataset","description":"$p_{\\mathrm T}$-differential yield of $\\phi$ in p-Pb collisions at $\\sqrt{s_{\\mathrm{NN}}}~=~$8.16 TeV (Multiplicity class 40-60%).","name":"Table 14"},{"@id":"https://doi.org/10.17182/hepdata.136309.v1/t15","@type":"Dataset","description":"$p_{\\mathrm T}$-differential yield of $\\phi$ in p-Pb collisions at $\\sqrt{s_{\\mathrm{NN}}}~=~$8.16 TeV (Multiplicity class 60-80%).","name":"Table 15"},{"@id":"https://doi.org/10.17182/hepdata.136309.v1/t16","@type":"Dataset","description":"$p_{\\mathrm T}$-differential yield of $\\phi$ in p-Pb collisions at $\\sqrt{s_{\\mathrm{NN}}}~=~$8.16 TeV (Multiplicity class 80-100%).","name":"Table 16"},{"@id":"https://doi.org/10.17182/hepdata.136309.v1/t17","@type":"Dataset","description":"$p_{\\mathrm T}$-differential $R_{\\mathrm{pPb}}$ of K$^{*0}$ in p-Pb collisions at $\\sqrt{s_{\\mathrm{NN}}}~=~$8.16 TeV.","name":"Table 17"},{"@id":"https://doi.org/10.17182/hepdata.136309.v1/t18","@type":"Dataset","description":"$p_{\\mathrm T}$-differential $R_{\\mathrm{pPb}}$ of $\\phi$ in p-Pb collisions at $\\sqrt{s_{\\mathrm{NN}}}~=~$8.16 TeV.","name":"Table 18"},{"@id":"https://doi.org/10.17182/hepdata.136309.v1/t19","@type":"Dataset","description":"$p_{\\mathrm T}$-differential $R_{\\mathrm{pPb}}$ of K$^{*0}$ in p-Pb collisions at $\\sqrt{s_{\\mathrm{NN}}}~=~$5.02 TeV.","name":"Table 19"},{"@id":"https://doi.org/10.17182/hepdata.136309.v1/t20","@type":"Dataset","description":"$p_{\\mathrm T}$-differential $R_{\\mathrm{pPb}}$ of $\\phi$ in p-Pb collisions at $\\sqrt{s_{\\mathrm{NN}}}~=~$5.02 TeV.","name":"Table 20"},{"@id":"https://doi.org/10.17182/hepdata.136309.v1/t21","@type":"Dataset","description":"$p_{\\mathrm T}$-differential $R_{\\mathrm{pPb}}$ of $\\Xi$ in p-Pb collisions at $\\sqrt{s_{\\mathrm{NN}}}~=~$5.02 TeV.","name":"Table 21"},{"@id":"https://doi.org/10.17182/hepdata.136309.v1/t22","@type":"Dataset","description":"$p_{\\mathrm T}$-differential $R_{\\mathrm{pPb}}$ of $\\Omega$ in p-Pb collisions at $\\sqrt{s_{\\mathrm{NN}}}~=~$5.02 TeV.","name":"Table 22"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1946970?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/136309"}],"inLanguage":"en","name":"$\\mathrm{K}^{*}(\\mathrm{892})^{0}$ and $\\mathrm{\\phi(1020)}$ production in p-Pb collisions at $\\sqrt{s_{\\rm NN}}$ = 8.16 TeV","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1946970?version=1","version":1}