cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.77995.v1/t17
title: "Table 17" 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 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: 10.17182/hepdata.77995.v1/t18
title: "Table 18" 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 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/t20
title: "Table 20" 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$^{*0}/\pi$ 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/t21
title: "Table 21" 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$^{*0}/\pi$ 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: 10.17182/hepdata.77995.v1/t22
title: "Table 22" 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: $\phi$/$\pi$ 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/t23
title: "Table 23" 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: $\phi$/$\pi$ 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: 10.17182/hepdata.77995.v1/t24
title: "Table 24" 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: p/K$^{*0}$ 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/t25
title: "Table 25" 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: p/K$^{*0}$ ratio as a function of $p_{\rm T}$ 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/t26
title: "Table 26" 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: p/K$^{*0}$ 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: 10.17182/hepdata.77995.v1/t27
title: "Table 27" 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: p/$\phi$ 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/t28
title: "Table 28" 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: p/$\phi$ ratio as a function of $p_{\rm T}$ 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/t29
title: "Table 29" 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: p/$\phi$ 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: 10.17182/hepdata.77995.v1/t30
title: "Table 30" 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: Nuclear modification factor of average $K^{*0}$ and $\overline{K^{*0}}$ 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: 10.5064/f6g2petf/p9glcn
title: Moore-et-al_MD_0521_Maryland Department of Health GoVAX Mobile COVID-19 vaccine clinic visits Lakeforest Mall in Gaithersburg.pdf
DOI: 10.17182/hepdata.77995.v1/t31
title: "Table 31" 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: Nuclear modification factor of average $K^{*0}$ and $\overline{K^{*0}}$ as a function of $p_{\rm T}$ for 5-10$\%$ 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/t32
title: "Table 32" 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: Nuclear modification factor of average $K^{*0}$ and $\overline{K^{*0}}$ as a function of $p_{\rm T}$ 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/t33
title: "Table 33" 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: Nuclear modification factor of average $K^{*0}$ and $\overline{K^{*0}}$ as a function of $p_{\rm T}$ 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/t34
title: "Table 34" 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: Nuclear modification factor of $\phi$ as a function of $p_{\rm T}$ for 0-5$\%$ 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/t35
title: "Table 35" 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: Nuclear modification factor of $\phi$ as a function of $p_{\rm T}$ for 5-10$\%$ 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/t36
title: "Table 36" 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: Nuclear modification factor of $\phi$ as a function of $p_{\rm T}$ for 20-30$\%$ 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/t37
title: "Table 37" 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: Nuclear modification factor of $\phi$ as a function of $p_{\rm T}$ for 40-50$\%$ 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.71277.v1/t1
title: "Table 1" of "Measurement of D$_s^+$ production and nuclear modification factor in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=2.76$ TeV"

description: $p_{\rm T}$-differential yield of prompt D$_s^+$ mesons in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$=2.76 TeV in the centrality class 0-10% in the rapidity interval |y|&lt;0.5.
Branching ratio of D$_s^+$-&gt;$\phi\pi^+$-&gt;$K^+K^-\pi^+$ : 0.0224.
The second (sys) error is the systematic uncertainty from the B feed-down contribution.
The first (sys) error is the systematic uncertainty from the other sources.
description: CERN-LHC. The production of prompt D$_s^+$ mesons was measured for the first time in collisions of heavy nuclei with the ALICE detector at the LHC. The analysis was performed on a data sample of Pb-Pb collisions at a centre-of-mass energy per nucleon pair, $\sqrt{s_{\rm NN}}$, of 2.76 TeV in two different centrality classes, namely 0-10% and 20-50%. The nuclear modification factor $R_{\rm AA}$ was computed by comparing the $p_{\rm T}$-differential production yields in Pb-Pb collisions to those in proton-proton (pp) collisions at the same energy. The production ratios D$_s^+$/D$^0$ and D$_s^+$\D$^+$ were also measured in Pb-Pb collisions and compared to their values in proton-proton collisions.
DOI: 10.17182/hepdata.71277.v1/t2
title: "Table 2" of "Measurement of D$_s^+$ production and nuclear modification factor in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=2.76$ TeV"

description: $p_{\rm T}$-differential yield of prompt D$_s^+$ mesons in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$=2.76 TeV in the centrality class 20-50% in the rapidity interval |y|&lt;0.5.
Branching ratio of D$_s^+$-&gt;$\phi\pi^+$-&gt;$K^+K^-\pi^+$ : 0.0224.
The second (sys) error is the systematic uncertainty from the B feed-down contribution.
The first (sys) error is the systematic uncertainty from the other sources.
description: CERN-LHC. The production of prompt D$_s^+$ mesons was measured for the first time in collisions of heavy nuclei with the ALICE detector at the LHC. The analysis was performed on a data sample of Pb-Pb collisions at a centre-of-mass energy per nucleon pair, $\sqrt{s_{\rm NN}}$, of 2.76 TeV in two different centrality classes, namely 0-10% and 20-50%. The nuclear modification factor $R_{\rm AA}$ was computed by comparing the $p_{\rm T}$-differential production yields in Pb-Pb collisions to those in proton-proton (pp) collisions at the same energy. The production ratios D$_s^+$/D$^0$ and D$_s^+$\D$^+$ were also measured in Pb-Pb collisions and compared to their values in proton-proton collisions.