{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.133031.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/2070441"}},{"@id":"https://doi.org/10.1140/epjc/s10052-023-11449-3","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ALICE Collaboration"},"creator":{"@type":"Organization","name":"ALICE Collaboration"},"datePublished":"2022","description":"The transverse-momentum ($p_{\\rm T}$) spectra of ${\\rm K}^*(892)^0$ and $\\phi(1020)$ measured with the ALICE detector up to $p_{\\rm T}$ = 16 GeV/$c$ in the rapidity range $-1.2 < y < 0.3$, in p-Pb collisions at the center-of-mass energy per nucleon-nucleon collision $\\sqrt{s_{\\rm NN}}$ = 5.02 TeV are presented as a function of charged particle multiplicity and rapidity. The measured $p_{\\rm T}$ distributions show a dependence on both multiplicity and rapidity at low $p_{\\rm T}$ whereas no significant dependence is observed at high $p_{\\rm T}$. A rapidity dependence is observed in the $p_{\\rm T}$-integrated yield (d$N$/d$y$), whereas the mean transverse momentum ($\\left< p_{\\rm T} \\right>$) shows a flat behavior as a function of rapidity. The rapidity asymmetry ($Y_{\\rm asym}$) at low $p_{\\rm T}$ ( < 5 GeV/$c$) is more significant for higher multiplicity classes. At high $p_{\\rm T}$, no significant rapidity asymmetry is observed in any of the multiplicity classes. Both ${\\rm K}^*(892)^0$ and $\\phi(1020)$ show similar $Y_{\\rm asym}$. The nuclear modification factor ($Q_{\\rm CP}$) as a function of $p_{\\rm T}$ shows a Cronin-like enhancement at intermediate $p_{\\rm T}$, which is more prominent at higher rapidities (Pb-going direction) and in higher multiplicity classes. At high $p_{\\rm T}$ (> 5 GeV/$c$), the $Q_{\\rm CP}$ values are greater than unity and no significant rapidity dependence is observed.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.133031.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}}}~=~$5.02 TeV ($0.0 &lt; y &lt; 0.3$).","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.133031.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}}}~=~$5.02 TeV ($-0.3 &lt; y &lt; 0.0$).","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.133031.v1/t3","@type":"Dataset","description":"$p_{\\mathrm T}$-differential yield of $\\frac{\\mathrm{K^{*0}} + \\overline{\\mathrm{K^{*0}}}}{2}$ in p-Pb collisions at $\\sqrt{s_{\\mathrm{NN}}}~=~$5.02 TeV ($-0.6 &lt; y &lt; -0.3$).","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.133031.v1/t4","@type":"Dataset","description":"$p_{\\mathrm T}$-differential yield of $\\frac{\\mathrm{K^{*0}} + \\overline{\\mathrm{K^{*0}}}}{2}$ in p-Pb collisions at $\\sqrt{s_{\\mathrm{NN}}}~=~$5.02 TeV ($-0.9 &lt; y &lt; -0.6$).","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.133031.v1/t5","@type":"Dataset","description":"$p_{\\mathrm T}$-differential yield of $\\frac{\\mathrm{K^{*0}} + \\overline{\\mathrm{K^{*0}}}}{2}$ in p-Pb collisions at $\\sqrt{s_{\\mathrm{NN}}}~=~$5.02 TeV ($-1.2 &lt; y &lt; -0.9$).","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.133031.v1/t6","@type":"Dataset","description":"$p_{\\mathrm T}$-differential yield of $\\phi$ in p-Pb collisions at $\\sqrt{s_{\\mathrm{NN}}}~=~$5.02 TeV ($0.0 &lt; y &lt; 0.3$).","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.133031.v1/t7","@type":"Dataset","description":"$p_{\\mathrm T}$-differential yield of $\\phi$ in p-Pb collisions at $\\sqrt{s_{\\mathrm{NN}}}~=~$5.02 TeV ($-0.3 &lt; y &lt; 0.0$).","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.133031.v1/t8","@type":"Dataset","description":"$p_{\\mathrm T}$-differential yield of $\\phi$ in p-Pb collisions at $\\sqrt{s_{\\mathrm{NN}}}~=~$5.02 TeV ($-0.6 &lt; y &lt; -0.3$).","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.133031.v1/t9","@type":"Dataset","description":"$p_{\\mathrm T}$-differential yield of $\\phi$ in p-Pb collisions at $\\sqrt{s_{\\mathrm{NN}}}~=~$5.02 TeV ($-0.9 &lt; y &lt; -0.6$).","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.133031.v1/t10","@type":"Dataset","description":"$p_{\\mathrm T}$-differential yield of $\\phi$ in p-Pb collisions at $\\sqrt{s_{\\mathrm{NN}}}~=~$5.02 TeV ($-1.2 &lt; y &lt; -0.9$).","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.133031.v1/t11","@type":"Dataset","description":"d$N$/d$y$ of $\\frac{\\mathrm{K^{*0}} + \\overline{\\mathrm{K^{*0}}}}{2}$ in p-Pb collisions at $\\sqrt{s_{\\mathrm{NN}}}~=~$5.02 TeV (V0A multiplicity classes).","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.133031.v1/t12","@type":"Dataset","description":"d$N$/d$y$ of $\\phi$ in p-Pb collisions at $\\sqrt{s_{\\mathrm{NN}}}~=~$5.02 TeV (V0A multiplicity classes).","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.133031.v1/t13","@type":"Dataset","description":"$\\langle p_\\mathrm{T}\\rangle$ of $\\frac{\\mathrm{K^{*0}} + \\overline{\\mathrm{K^{*0}}}}{2}$ in p-Pb collisions at $\\sqrt{s_{\\mathrm{NN}}}~=~$5.02 TeV (V0A multiplicity classes).","name":"Table 13"},{"@id":"https://doi.org/10.17182/hepdata.133031.v1/t14","@type":"Dataset","description":"$\\langle p_\\mathrm{T}\\rangle$ of $\\phi$ in p-Pb collisions at $\\sqrt{s_{\\mathrm{NN}}}~=~$5.02 TeV (V0A multiplicity classes).","name":"Table 14"},{"@id":"https://doi.org/10.17182/hepdata.133031.v1/t15","@type":"Dataset","description":"(d$N$/$\\mathrm{d}y$)/(d$N$/$\\mathrm{d}y)_{y=0}$ of $\\frac{\\mathrm{K^{*0}} + \\overline{\\mathrm{K^{*0}}}}{2}$ in p-Pb collisions at $\\sqrt{s_{\\mathrm{NN}}}~=~$5.02 TeV (0-100 %).","name":"Table 15"},{"@id":"https://doi.org/10.17182/hepdata.133031.v1/t16","@type":"Dataset","description":"(d$N$/$\\mathrm{d}y$)/(d$N$/$\\mathrm{d}y)_{y=0}$ of $\\phi$ in p-Pb collisions at $\\sqrt{s_{\\mathrm{NN}}}~=~$5.02 TeV (0-100 %).","name":"Table 16"},{"@id":"https://doi.org/10.17182/hepdata.133031.v1/t17","@type":"Dataset","description":"$\\langle p_\\mathrm{T}\\rangle_\\mathrm{y}$/$\\langle p_\\mathrm{T}\\rangle_\\mathrm{y=0}$ of $\\frac{\\mathrm{K^{*0}} + \\overline{\\mathrm{K^{*0}}}}{2}$ in p-Pb collisions at $\\sqrt{s_{\\mathrm{NN}}}~=~$5.02 TeV (0-100 %).","name":"Table 17"},{"@id":"https://doi.org/10.17182/hepdata.133031.v1/t18","@type":"Dataset","description":"$\\langle p_\\mathrm{T}\\rangle_\\mathrm{y}$/$\\langle p_\\mathrm{T}\\rangle_\\mathrm{y=0}$ of $\\phi$ in p-Pb collisions at $\\sqrt{s_{\\mathrm{NN}}}~=~$5.02 TeV (0-100%).","name":"Table 18"},{"@id":"https://doi.org/10.17182/hepdata.133031.v1/t19","@type":"Dataset","description":"$y_{asym}$ of $\\frac{\\mathrm{K^{*0}} + \\overline{\\mathrm{K^{*0}}}}{2}$ in p-Pb collisions at $\\sqrt{s_{\\mathrm{NN}}}~=~$5.02 TeV (V0A multiplicity classes).","name":"Table 19"},{"@id":"https://doi.org/10.17182/hepdata.133031.v1/t20","@type":"Dataset","description":"$y_{asym}$ of $\\phi$ in p-Pb collisions at $\\sqrt{s_{\\mathrm{NN}}}~=~$5.02 TeV (V0A multiplicity classes).","name":"Table 20"},{"@id":"https://doi.org/10.17182/hepdata.133031.v1/t21","@type":"Dataset","description":"$Q_{CP}$ of $\\frac{\\mathrm{K^{*0}} + \\overline{\\mathrm{K^{*0}}}}{2}$ in p-Pb collisions at $\\sqrt{s_{\\mathrm{NN}}}~=~$5.02 TeV (0-10 %/40-100 %).","name":"Table 21"},{"@id":"https://doi.org/10.17182/hepdata.133031.v1/t22","@type":"Dataset","description":"$Q_{CP}$ of $\\phi$ in p-Pb collisions at $\\sqrt{s_{\\mathrm{NN}}}~=~$5.02 TeV (0-10 %/40-100%).","name":"Table 22"},{"@id":"https://doi.org/10.17182/hepdata.133031.v1/t23","@type":"Dataset","description":"$Q_{CP}$ of $\\frac{\\mathrm{K^{*0}} + \\overline{\\mathrm{K^{*0}}}}{2}$ in p-Pb collisions at $\\sqrt{s_{\\mathrm{NN}}}~=~$5.02 TeV (10-40 %/40-100 %).","name":"Table 23"},{"@id":"https://doi.org/10.17182/hepdata.133031.v1/t24","@type":"Dataset","description":"$Q_{CP}$ of $\\phi$ in p-Pb collisions at $\\sqrt{s_{\\mathrm{NN}}}~=~$5.02 TeV (10-40 %/40-100%).","name":"Table 24"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins2070441?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/133031"}],"inLanguage":"en","name":"Multiplicity and rapidity dependence of ${\\rm K}^*(892)^0$ and $\\phi(1020)$ production in p-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/ins2070441?version=1","version":1}