cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.73306.v1/t5
title: "Table 5" of "Centrality dependence of $\mathbf{\psi}$(2S) suppression in p-Pb collisions at $\mathbf{\sqrt{{\textit s}_{\rm NN}}}$ = 5.02 TeV"

description: Centrality dependence of the Psi(2S) Q_pPb in the forward rapidity range (2.03
description: CERN-LHC. The inclusive production of the $\psi$(2S) charmonium state was studied as a function of centrality in p-Pb collisions at the nucleon-nucleon center of mass energy $\sqrt{s_{\rm NN}}$ = 5.02 TeV at the CERN LHC. The measurement was performed with the ALICE detector in the center of mass rapidity ranges $-4.46
DOI: 10.17182/hepdata.73306.v1/t6
title: "Table 6" of "Centrality dependence of $\mathbf{\psi}$(2S) suppression in p-Pb collisions at $\mathbf{\sqrt{{\textit s}_{\rm NN}}}$ = 5.02 TeV"

description: Psi(2S)/J/Psi)_pA/(Psi(2S)/J/Psi)_pp double ratio in the backward rapidity range (-4.46
description: CERN-LHC. The inclusive production of the $\psi$(2S) charmonium state was studied as a function of centrality in p-Pb collisions at the nucleon-nucleon center of mass energy $\sqrt{s_{\rm NN}}$ = 5.02 TeV at the CERN LHC. The measurement was performed with the ALICE detector in the center of mass rapidity ranges $-4.46
DOI: 10.17182/hepdata.73306.v1/t7
title: "Table 7" of "Centrality dependence of $\mathbf{\psi}$(2S) suppression in p-Pb collisions at $\mathbf{\sqrt{{\textit s}_{\rm NN}}}$ = 5.02 TeV"

description: Psi(2S)/J/Psi)_pA/(Psi(2S)/J/Psi)_pp double ratio in the forward rapidity range (2.03
description: CERN-LHC. The inclusive production of the $\psi$(2S) charmonium state was studied as a function of centrality in p-Pb collisions at the nucleon-nucleon center of mass energy $\sqrt{s_{\rm NN}}$ = 5.02 TeV at the CERN LHC. The measurement was performed with the ALICE detector in the center of mass rapidity ranges $-4.46
DOI: 10.17182/hepdata.80796.v1/t1
title: "Table 1" of "Evolution of the longitudinal and azimuthal structure of the near-side jet peak in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV"

description: Variance of the near-side jet peak from a generalized Gaussian fit.
description: CERN-LHC. The evolution of the near-side jet peak is studied in Pb-Pb collisions at 2.76 TeV as a function of centrality and $p_{\rm T}$ and in pp collisions at the same energy as a function of $p_{\rm T}$.
DOI: 10.5064/f6g2petf/fila2u
title: Moore-et-al_MD_0521_Governor Larry Hogan - Official Website for the Governor of Maryland_14.pdf
DOI: 10.17182/hepdata.77995.v1/t1
title: "Table 1" of "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"

description: Invariant yield of K$^{*0}$ meson normalized to the number of inelastic pp collisions at $\sqrt{s}=2.76~{\rm TeV}$.
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 $|y|&lt;0.5$ 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.
DOI: 10.17182/hepdata.77995.v1/t2
title: "Table 2" of "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"

description: Invariant yield of $\phi$ meson normalized to the number of inelastic pp collisions at $\sqrt{s}=2.76~{\rm TeV}$.
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 $|y|&lt;0.5$ 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.
DOI: 10.17182/hepdata.80796.v1/t2
title: "Table 2" of "Evolution of the longitudinal and azimuthal structure of the near-side jet peak in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV"

description: Variance of the near-side jet peak from a generalized Gaussian fit.
description: CERN-LHC. The evolution of the near-side jet peak is studied in Pb-Pb collisions at 2.76 TeV as a function of centrality and $p_{\rm T}$ and in pp collisions at the same energy as a function of $p_{\rm T}$.
DOI: 10.17182/hepdata.80796.v1/t3
title: "Table 3" of "Evolution of the longitudinal and azimuthal structure of the near-side jet peak in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV"

description: Variance of near-side peak in the 0-10% centrality bin divided by the variance of the near-side peak in the 50-80% centrality bin.
description: CERN-LHC. The evolution of the near-side jet peak is studied in Pb-Pb collisions at 2.76 TeV as a function of centrality and $p_{\rm T}$ and in pp collisions at the same energy as a function of $p_{\rm T}$.
DOI: 10.17182/hepdata.80796.v1/t4
title: "Table 4" of "Evolution of the longitudinal and azimuthal structure of the near-side jet peak in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV"

description: Variance of near-side peak in the 0-10% centrality bin divided by the variance of the near-side peak in the 50-80% centrality bin.
description: CERN-LHC. The evolution of the near-side jet peak is studied in Pb-Pb collisions at 2.76 TeV as a function of centrality and $p_{\rm T}$ and in pp collisions at the same energy as a function of $p_{\rm T}$.
DOI: 10.17182/hepdata.80796.v1/t5
title: "Table 5" of "Evolution of the longitudinal and azimuthal structure of the near-side jet peak in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV"

description: Depletion yield calculated by taking the difference of the fit and the data, and normalized by the total yield of the peak.
description: CERN-LHC. The evolution of the near-side jet peak is studied in Pb-Pb collisions at 2.76 TeV as a function of centrality and $p_{\rm T}$ and in pp collisions at the same energy as a function of $p_{\rm T}$.
DOI: 10.17182/hepdata.80796.v1/t6
title: "Table 6" of "Evolution of the longitudinal and azimuthal structure of the near-side jet peak in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV"

description: Variance of the near-side jet peak from a generalized Gaussian fit.
description: CERN-LHC. The evolution of the near-side jet peak is studied in Pb-Pb collisions at 2.76 TeV as a function of centrality and $p_{\rm T}$ and in pp collisions at the same energy as a function of $p_{\rm T}$.
DOI: 10.17182/hepdata.80796.v1/t7
title: "Table 7" of "Evolution of the longitudinal and azimuthal structure of the near-side jet peak in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV"

description: Variance of the near-side jet peak from a generalized Gaussian fit.
description: CERN-LHC. The evolution of the near-side jet peak is studied in Pb-Pb collisions at 2.76 TeV as a function of centrality and $p_{\rm T}$ and in pp collisions at the same energy as a function of $p_{\rm T}$.
DOI: 10.17182/hepdata.77995.v1/t10
title: "Table 10" of "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"

description: Invariant yield of $\phi$ meson for 5-10$\%$ centrality in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=2.76~{\rm TeV}$.
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 $|y|&lt;0.5$ 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.
DOI: 10.17182/hepdata.77995.v1/t3
title: "Table 3" of "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"

description: Invariant yield of K$^{*0}$ meson for 0-5$\%$ centrality in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=2.76~{\rm TeV}$.
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 $|y|&lt;0.5$ 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.
DOI: 10.17182/hepdata.77995.v1/t4
title: "Table 4" of "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"

description: Invariant yield of K$^{*0}$ meson for 5-10$\%$ centrality in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=2.76~{\rm TeV}$.
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 $|y|&lt;0.5$ 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.
DOI: 10.17182/hepdata.77995.v1/t5
title: "Table 5" of "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"

description: Invariant yield of K$^{*0}$ meson for 10-20$\%$ centrality in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=2.76~{\rm TeV}$.
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 $|y|&lt;0.5$ 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.
DOI: 10.17182/hepdata.77995.v1/t6
title: "Table 6" of "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"

description: Invariant yield of K$^{*0}$ meson for 20-30$\%$ centrality in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=2.76~{\rm TeV}$.
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 $|y|&lt;0.5$ 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.
DOI: 10.17182/hepdata.77995.v1/t7
title: "Table 7" of "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"

description: Invariant yield of K$^{*0}$ meson for 30-40$\%$ centrality in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=2.76~{\rm TeV}$.
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 $|y|&lt;0.5$ 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.
DOI: 10.17182/hepdata.77995.v1/t8
title: "Table 8" of "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"

description: Invariant yield of K$^{*0}$ meson for 40-50$\%$ centrality in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=2.76~{\rm TeV}$.
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 $|y|&lt;0.5$ 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.
DOI: 10.17182/hepdata.77995.v1/t9
title: "Table 9" of "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"

description: Invariant yield of $\phi$ meson for 0-5$\%$ centrality in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=2.76~{\rm TeV}$.
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 $|y|&lt;0.5$ 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.
DOI: 10.17182/hepdata.77995.v1/t11
title: "Table 11" of "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"

description: Invariant yield of $\phi$ meson for 10-20$\%$ centrality in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=2.76~{\rm TeV}$.
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 $|y|&lt;0.5$ 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.
DOI: 10.17182/hepdata.77995.v1/t12
title: "Table 12" of "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"

description: Invariant yield of $\phi$ meson for 20-30$\%$ centrality in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=2.76~{\rm TeV}$.
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 $|y|&lt;0.5$ 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.
DOI: 10.17182/hepdata.77995.v1/t13
title: "Table 13" of "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"

description: Invariant yield of $\phi$ meson for 30-40$\%$ centrality in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=2.76~{\rm TeV}$.
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 $|y|&lt;0.5$ 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.
DOI: 10.17182/hepdata.77995.v1/t14
title: "Table 14" of "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"

description: Invariant yield of $\phi$ meson for 40-50$\%$ centrality in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=2.76~{\rm TeV}$.
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 $|y|&lt;0.5$ 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.
DOI: 10.17182/hepdata.77995.v1/t15
title: "Table 15" of "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"

description: Invariant yield of $\phi$ meson for 60-80$\%$ centrality in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=2.76~{\rm TeV}$.
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 $|y|&lt;0.5$ 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.
DOI: 10.17182/hepdata.77995.v1/t16
title: "Table 16" of "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"

description: K$^{*0}$/K ratio as a function of $p_{\rm T}$ for 0-5$\%$ centrality in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=2.76~{\rm TeV}$.
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 $|y|&lt;0.5$ 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.
DOI: 10.17182/hepdata.77995.v1/t19
title: "Table 19" of "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"

description: $\phi$/K ratio as a function of $p_{\rm T}$ for inelastic (INEL) pp collisions at $\sqrt{s}=2.76~{\rm TeV}$.
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 $|y|&lt;0.5$ 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.
DOI: 10.5064/f6g2petf/w0jm73
title: Moore-et-al_MD_0521_Governor Larry Hogan - Official Website for the Governor of Maryland_03.pdf