cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.100595.v1/t9
title: "Figure 9-1" of "K*(892) resonance production in Au + Au and p + p collisions at s(NN)**(1/2) = 200-GeV at STAR."

description: The $K^{*0}$ and $K^{*\pm}$ reconstruction efficiency multiplied by the detector acceptance as a function of $p_T$ in minimum bias $p + p$ and different centralities in Au+Au collisions.
description: The short-lived $K(892)^*$ resonance provides an efficient tool to probe properties of the hot and dense medium produced in relativistic heavy-ion collisions. We report measurements of $K^*$ in $sqrt{s_{NN}} =200GeV$ Au+Au and $p+p$ collisions reconstructed via its hadronic decay channels $K(892)^{*0}-&gt;K\pi$ and $K(892)^{*\pm}-&gt;K_S^0\pi^{\pm}$ using the STAR detector at RHIC. The $K^{*0}$ mass has been studied as a function of $p_T$ in minimum bias $p+p$ and central Au+Au collisions. The $K^*$ $p_T$ spectra for minimum bias $p+p$ interactions and for Au+Au collisions in different centralities are presented. The $K^*/K$ yield ratios for all centralities in Au+Au collisions are found to be significantly lower than the ratio in minimum bias $p+p$ collisions, indicating the importance of hadronic interactions between chemical and kinetic freeze-outs. A significant non-zero $K^{*0}$ elliptic flow ($v^2$) is observed in Au+Au collisions and compared to the $K_S^0$ and $\Lambda$ $v^2$. The nuclear modification factor of $K^*$ at intermediate $p_T$ is similar to that of $K_S^0$ , but different from $\Lambda$. This establishes a baryon-meson effect over a mass effect in the particle production at intermediate pT (2
DOI: 10.17182/hepdata.100595.v1/t16
title: "Figure 11-1" of "K*(892) resonance production in Au + Au and p + p collisions at s(NN)**(1/2) = 200-GeV at STAR."

description: (Color online) The invariant yields for both $(K^{*0} + \bar{K^{*0}})/2$ and $(K^{*+} + K^{*-})/2$ as a function of $p_T$ for |y| &lt; 0.5 in minimum bias $p + p$ interactions. The dotted curve is the fit to the power-law function from Equation 13 for $p_T$ &gt; 0.5 GeV/$c$ and extended to lower values of $p_T$ . The dashed curve is the $K^{*0}$ spectrum fit to the exponential function from Equation 12 and extended to higher values of $p_T$ . The dashed-dotted curve is the fit to the Levy function from Equation 14 for $p_T$ &lt; 4 GeV/$c$. Errors are statistical only.
description: The short-lived $K(892)^*$ resonance provides an efficient tool to probe properties of the hot and dense medium produced in relativistic heavy-ion collisions. We report measurements of $K^*$ in $sqrt{s_{NN}} =200GeV$ Au+Au and $p+p$ collisions reconstructed via its hadronic decay channels $K(892)^{*0}-&gt;K\pi$ and $K(892)^{*\pm}-&gt;K_S^0\pi^{\pm}$ using the STAR detector at RHIC. The $K^{*0}$ mass has been studied as a function of $p_T$ in minimum bias $p+p$ and central Au+Au collisions. The $K^*$ $p_T$ spectra for minimum bias $p+p$ interactions and for Au+Au collisions in different centralities are presented. The $K^*/K$ yield ratios for all centralities in Au+Au collisions are found to be significantly lower than the ratio in minimum bias $p+p$ collisions, indicating the importance of hadronic interactions between chemical and kinetic freeze-outs. A significant non-zero $K^{*0}$ elliptic flow ($v^2$) is observed in Au+Au collisions and compared to the $K_S^0$ and $\Lambda$ $v^2$. The nuclear modification factor of $K^*$ at intermediate $p_T$ is similar to that of $K_S^0$ , but different from $\Lambda$. This establishes a baryon-meson effect over a mass effect in the particle production at intermediate pT (2
DOI: 10.17182/hepdata.100595.v1/t17
title: "Figure 11-2" of "K*(892) resonance production in Au + Au and p + p collisions at s(NN)**(1/2) = 200-GeV at STAR."

description: (Color online) The invariant yields for both $(K^{*0} + \bar{K^{*0}})/2$ and $(K^{*+} + K^{*-})/2$ as a function of $p_T$ for |y| &lt; 0.5 in minimum bias $p + p$ interactions. The dotted curve is the fit to the power-law function from Equation 13 for $p_T$ &gt; 0.5 GeV/$c$ and extended to lower values of $p_T$ . The dashed curve is the $K^{*0}$ spectrum fit to the exponential function from Equation 12 and extended to higher values of $p_T$ . The dashed-dotted curve is the fit to the Levy function from Equation 14 for $p_T$ &lt; 4 GeV/$c$. Errors are statistical only.
description: The short-lived $K(892)^*$ resonance provides an efficient tool to probe properties of the hot and dense medium produced in relativistic heavy-ion collisions. We report measurements of $K^*$ in $sqrt{s_{NN}} =200GeV$ Au+Au and $p+p$ collisions reconstructed via its hadronic decay channels $K(892)^{*0}-&gt;K\pi$ and $K(892)^{*\pm}-&gt;K_S^0\pi^{\pm}$ using the STAR detector at RHIC. The $K^{*0}$ mass has been studied as a function of $p_T$ in minimum bias $p+p$ and central Au+Au collisions. The $K^*$ $p_T$ spectra for minimum bias $p+p$ interactions and for Au+Au collisions in different centralities are presented. The $K^*/K$ yield ratios for all centralities in Au+Au collisions are found to be significantly lower than the ratio in minimum bias $p+p$ collisions, indicating the importance of hadronic interactions between chemical and kinetic freeze-outs. A significant non-zero $K^{*0}$ elliptic flow ($v^2$) is observed in Au+Au collisions and compared to the $K_S^0$ and $\Lambda$ $v^2$. The nuclear modification factor of $K^*$ at intermediate $p_T$ is similar to that of $K_S^0$ , but different from $\Lambda$. This establishes a baryon-meson effect over a mass effect in the particle production at intermediate pT (2
DOI: 10.17182/hepdata.100595.v1/t18
title: "Figure 12" of "K*(892) resonance production in Au + Au and p + p collisions at s(NN)**(1/2) = 200-GeV at STAR."

description: (Color online) The $K^*$ $$ as a function of $dN_{ch}/d\eta$ compared to that of $\pi^−$, $K^−$, and $p$ for minimum bias $p+p$ (solid symbols) and Au+Au (open symbols) collisions. The errors shown are the quadratic sum of the statistical and systematic uncertainties.
description: The short-lived $K(892)^*$ resonance provides an efficient tool to probe properties of the hot and dense medium produced in relativistic heavy-ion collisions. We report measurements of $K^*$ in $sqrt{s_{NN}} =200GeV$ Au+Au and $p+p$ collisions reconstructed via its hadronic decay channels $K(892)^{*0}-&gt;K\pi$ and $K(892)^{*\pm}-&gt;K_S^0\pi^{\pm}$ using the STAR detector at RHIC. The $K^{*0}$ mass has been studied as a function of $p_T$ in minimum bias $p+p$ and central Au+Au collisions. The $K^*$ $p_T$ spectra for minimum bias $p+p$ interactions and for Au+Au collisions in different centralities are presented. The $K^*/K$ yield ratios for all centralities in Au+Au collisions are found to be significantly lower than the ratio in minimum bias $p+p$ collisions, indicating the importance of hadronic interactions between chemical and kinetic freeze-outs. A significant non-zero $K^{*0}$ elliptic flow ($v^2$) is observed in Au+Au collisions and compared to the $K_S^0$ and $\Lambda$ $v^2$. The nuclear modification factor of $K^*$ at intermediate $p_T$ is similar to that of $K_S^0$ , but different from $\Lambda$. This establishes a baryon-meson effect over a mass effect in the particle production at intermediate pT (2
DOI: 10.17182/hepdata.100595.v1/t19
title: "Figure 13-1" of "K*(892) resonance production in Au + Au and p + p collisions at s(NN)**(1/2) = 200-GeV at STAR."

description: The $K^*/K$ (upper panel) and $\phi/K^*$ (lower panel) yield ratios as a function of the c.m. system energies. The yield ratios for central Au+Au collisions at $\sqrt{s_{NN}}$=130 [35] and 200 GeV and minimum bias $p+p$ interactions at $\sqrt{s_{NN}}$=200 GeV are compared to measurements from e+e- at sqrt(s) of 10.45 GeV [48], 29 GeV [49] and 91 GeV [50,51], pbar-p at sqrt(s) of 5.6 GeV [52] and pp at sqrt(s) of 27.5 GeV [53], 52.5 GeV [54] and 63 GeV [55]. The errors at $\sqrt{s_{NN}}$=130 and 200 GeV correspond to the quadratic sum of the statistical and systematic errors.
description: The short-lived $K(892)^*$ resonance provides an efficient tool to probe properties of the hot and dense medium produced in relativistic heavy-ion collisions. We report measurements of $K^*$ in $sqrt{s_{NN}} =200GeV$ Au+Au and $p+p$ collisions reconstructed via its hadronic decay channels $K(892)^{*0}-&gt;K\pi$ and $K(892)^{*\pm}-&gt;K_S^0\pi^{\pm}$ using the STAR detector at RHIC. The $K^{*0}$ mass has been studied as a function of $p_T$ in minimum bias $p+p$ and central Au+Au collisions. The $K^*$ $p_T$ spectra for minimum bias $p+p$ interactions and for Au+Au collisions in different centralities are presented. The $K^*/K$ yield ratios for all centralities in Au+Au collisions are found to be significantly lower than the ratio in minimum bias $p+p$ collisions, indicating the importance of hadronic interactions between chemical and kinetic freeze-outs. A significant non-zero $K^{*0}$ elliptic flow ($v^2$) is observed in Au+Au collisions and compared to the $K_S^0$ and $\Lambda$ $v^2$. The nuclear modification factor of $K^*$ at intermediate $p_T$ is similar to that of $K_S^0$ , but different from $\Lambda$. This establishes a baryon-meson effect over a mass effect in the particle production at intermediate pT (2
DOI: 10.17182/hepdata.100595.v1/t20
title: "Figure 13-2" of "K*(892) resonance production in Au + Au and p + p collisions at s(NN)**(1/2) = 200-GeV at STAR."

description: The $K^*/K$ (upper panel) and $\phi/K^*$ (lower panel) yield ratios as a function of the c.m. system energies. The yield ratios for central Au+Au collisions at $\sqrt{s_{NN}}$=130 [35] and 200 GeV and minimum bias $p+p$ interactions at $\sqrt{s_{NN}}$=200 GeV are compared to measurements from e+e- at sqrt(s) of 10.45 GeV [48], 29 GeV [49] and 91 GeV [50,51], pbar-p at sqrt(s) of 5.6 GeV [52] and pp at sqrt(s) of 27.5 GeV [53], 52.5 GeV [54] and 63 GeV [55]. The errors at $\sqrt{s_{NN}}$=130 and 200 GeV correspond to the quadratic sum of the statistical and systematic errors.
description: The short-lived $K(892)^*$ resonance provides an efficient tool to probe properties of the hot and dense medium produced in relativistic heavy-ion collisions. We report measurements of $K^*$ in $sqrt{s_{NN}} =200GeV$ Au+Au and $p+p$ collisions reconstructed via its hadronic decay channels $K(892)^{*0}-&gt;K\pi$ and $K(892)^{*\pm}-&gt;K_S^0\pi^{\pm}$ using the STAR detector at RHIC. The $K^{*0}$ mass has been studied as a function of $p_T$ in minimum bias $p+p$ and central Au+Au collisions. The $K^*$ $p_T$ spectra for minimum bias $p+p$ interactions and for Au+Au collisions in different centralities are presented. The $K^*/K$ yield ratios for all centralities in Au+Au collisions are found to be significantly lower than the ratio in minimum bias $p+p$ collisions, indicating the importance of hadronic interactions between chemical and kinetic freeze-outs. A significant non-zero $K^{*0}$ elliptic flow ($v^2$) is observed in Au+Au collisions and compared to the $K_S^0$ and $\Lambda$ $v^2$. The nuclear modification factor of $K^*$ at intermediate $p_T$ is similar to that of $K_S^0$ , but different from $\Lambda$. This establishes a baryon-meson effect over a mass effect in the particle production at intermediate pT (2
DOI: 10.17182/hepdata.100595.v1/t21
title: "Figure 15" of "K*(892) resonance production in Au + Au and p + p collisions at s(NN)**(1/2) = 200-GeV at STAR."

description: The $K^{*0}$ v2 (filled stars) as a function of $p_T$ for minimum bias Au+Au collisions compared to the $K^{0}_S$ (open triangles), $\Lambda$ (open circles), and charged hadron (open diamonds) $v_2$. The errors shown are statistical only.
description: The short-lived $K(892)^*$ resonance provides an efficient tool to probe properties of the hot and dense medium produced in relativistic heavy-ion collisions. We report measurements of $K^*$ in $sqrt{s_{NN}} =200GeV$ Au+Au and $p+p$ collisions reconstructed via its hadronic decay channels $K(892)^{*0}-&gt;K\pi$ and $K(892)^{*\pm}-&gt;K_S^0\pi^{\pm}$ using the STAR detector at RHIC. The $K^{*0}$ mass has been studied as a function of $p_T$ in minimum bias $p+p$ and central Au+Au collisions. The $K^*$ $p_T$ spectra for minimum bias $p+p$ interactions and for Au+Au collisions in different centralities are presented. The $K^*/K$ yield ratios for all centralities in Au+Au collisions are found to be significantly lower than the ratio in minimum bias $p+p$ collisions, indicating the importance of hadronic interactions between chemical and kinetic freeze-outs. A significant non-zero $K^{*0}$ elliptic flow ($v^2$) is observed in Au+Au collisions and compared to the $K_S^0$ and $\Lambda$ $v^2$. The nuclear modification factor of $K^*$ at intermediate $p_T$ is similar to that of $K_S^0$ , but different from $\Lambda$. This establishes a baryon-meson effect over a mass effect in the particle production at intermediate pT (2
DOI: 10.17182/hepdata.101068.v1/t1
title: "Table 1" of "Net-proton number fluctuations and the Quantum Chromodynamics critical point"

description: Event-by-event net-proton multiplicity distributions for central (0-5$\%$) Au+Au collisions from $\sqrt{s_{NN}} = 7.7 - 200 GeV. The distributions are normalised to total number of events. The distributions are not corrected for proton and antiproton detection efficiency.
description: No data abstract available.
DOI: 10.17182/hepdata.100595.v1/t22
title: "Figure 16" of "K*(892) resonance production in Au + Au and p + p collisions at s(NN)**(1/2) = 200-GeV at STAR."

description: The $K^*$ $R_{AA}$ (filled triangles) and $R_{CP}$ (filled circles) as a function of $p_T$ compared to the $K^{0}_S$ (open circles) and $\Lambda$ (open triangles) $R_{CP}$. The errors shown are statistical only. The dashed line represents the number of binary collisions scaling. The widths of the grey bands represent the systematic uncertainties of $R_{AA}$ (left) and $R_{CP}$ (right) due to the model calculations of $N_{bin}$.
description: The short-lived $K(892)^*$ resonance provides an efficient tool to probe properties of the hot and dense medium produced in relativistic heavy-ion collisions. We report measurements of $K^*$ in $sqrt{s_{NN}} =200GeV$ Au+Au and $p+p$ collisions reconstructed via its hadronic decay channels $K(892)^{*0}-&gt;K\pi$ and $K(892)^{*\pm}-&gt;K_S^0\pi^{\pm}$ using the STAR detector at RHIC. The $K^{*0}$ mass has been studied as a function of $p_T$ in minimum bias $p+p$ and central Au+Au collisions. The $K^*$ $p_T$ spectra for minimum bias $p+p$ interactions and for Au+Au collisions in different centralities are presented. The $K^*/K$ yield ratios for all centralities in Au+Au collisions are found to be significantly lower than the ratio in minimum bias $p+p$ collisions, indicating the importance of hadronic interactions between chemical and kinetic freeze-outs. A significant non-zero $K^{*0}$ elliptic flow ($v^2$) is observed in Au+Au collisions and compared to the $K_S^0$ and $\Lambda$ $v^2$. The nuclear modification factor of $K^*$ at intermediate $p_T$ is similar to that of $K_S^0$ , but different from $\Lambda$. This establishes a baryon-meson effect over a mass effect in the particle production at intermediate pT (2
DOI: 10.17182/hepdata.101068.v1/t2
title: "Table 2" of "Net-proton number fluctuations and the Quantum Chromodynamics critical point"

description: Cumulants of net-proton distributions in Au+Au collisions for nine energies from $\sqrt{s_{NN}} = 7.7 - 200 GeV for 0-5$\%$ and 70-80$\%$ centrality.
description: No data abstract available.
DOI: 10.17182/hepdata.101068.v1/t3
title: "Table 3" of "Net-proton number fluctuations and the Quantum Chromodynamics critical point"

description: Cumulant ratios C3/C2 and C4/C2 of net-proton distributions in Au+Au collisions for eight energies from $\sqrt{s_{NN}} = 7.7 - 62.4 GeV for 0-5$\%$ centrality. Also given are the derivative of the polynomial fits to the C3/C2 and C4/C2 vs energy at each energy and the Skellam baselines for the ratios.
description: No data abstract available.
DOI: 10.17182/hepdata.101068.v1/t4
title: "Table 4" of "Net-proton number fluctuations and the Quantum Chromodynamics critical point"

description: Parameters of the polynomial fit of net-proton C3/C2 and C4/C2 vs energy in 0-5$\%$ central Au+Au collisions. Polynomial of order 5 and 4 are used to fit C3/C2 and C4/C2 ratio vs energies, respectively.
description: No data abstract available.
DOI: 10.17182/hepdata.101068.v1/t5
title: "Table 5" of "Net-proton number fluctuations and the Quantum Chromodynamics critical point"

description: Cumulant ratios C3/C2 and C4/C2 of net-proton distributions in STAR Au+Au collisions for nine energies from $\sqrt{s_{NN}} = 7.7 - 200 GeV for 0-5$\%$ and 70-80$\%$ centrality.
description: No data abstract available.
DOI: 10.17182/hepdata.101068.v1/t6
title: "Table 6" of "Net-proton number fluctuations and the Quantum Chromodynamics critical point"

description: Cumulant ratios C3/C2 and C4/C2 of net-proton distributions in Au+Au collisions from UrQMD for 0-5$\%$ centrality.
description: No data abstract available.
DOI: 10.17182/hepdata.101068.v1/t7
title: "Table 7" of "Net-proton number fluctuations and the Quantum Chromodynamics critical point"

description: Cumulant ratios C3/C2 and C4/C2 of net-proton distributions from HRG GCE, HRG GEC excluded volume, HRG CE model.
description: No data abstract available.
DOI: 10.17182/hepdata.101068.v1/t8
title: "Table 8" of "Net-proton number fluctuations and the Quantum Chromodynamics critical point"

description: Cumulants and their ratios up to fourth order in Au+Au collisions at $\sqrt{s_{NN}} = 200 GeV using conventional analytical efficiency corrections and unfolding approaches with various cases of distribution of detector response.
description: No data abstract available.
DOI: 10.17182/hepdata.101068.v1/t10
title: "Table 10" of "Net-proton number fluctuations and the Quantum Chromodynamics critical point"

description: Significance of deviations in net-proton C4/C2 (or kappa*sigma^2) for central 0-5$\%$ Au+Au collisions and those from UrQMD, HRG and peripheral 70-80$\%$ data.
description: No data abstract available.
DOI: 10.17182/hepdata.101068.v1/t9
title: "Table 9" of "Net-proton number fluctuations and the Quantum Chromodynamics critical point"

description: Rapidity dependence of cumulant ratio C4/C2 of net-proton distributions for 0-5$\%$ central Au+Au collisions at nine energies from $\sqrt{s_{NN}} = 7.7 - 200 GeV.
description: No data abstract available.
DOI: 10.17182/hepdata.101172.v1/t1
title: "Figure 1a" of "Observation of $D_{s}^{\pm}/D^0$ enhancement in Au+Au collisions at $\sqrt{s_{_{NN}}}$ = 200 GeV"

description: The $KK\pi$ invariant mass distribution (Counts per 8 MeV/$c^{2}$ bin) for right-sign combinations in 0-80% Au+Au collisions at $\sqrt{s_{_{\rm NN}}}$ = 200 GeV.
description: RHIC-BNL. We report on the first measurement of the charmed-strange meson
DOI: 10.17182/hepdata.101172.v1/t2
title: "Figure 1b (0-10%)" of "Observation of $D_{s}^{\pm}/D^0$ enhancement in Au+Au collisions at $\sqrt{s_{_{NN}}}$ = 200 GeV"

description: $D_s^{\pm}$ invariant yield as a function of $p_{T}$ in 0-10% centrality bin of Au+Au collisions at $\sqrt{s_{_{\rm NN}}}$ = 200 GeV. The $p_T$ bins are 1.5 &lt; $p_T$ &lt; 2.5 GeV/c, 2.5 &lt; $p_T$ &lt; 3.5 GeV/c, 3.5 &lt; $p_T$ &lt; 5.0 GeV/c and 5.0 &lt; $p_T$ &lt; 8.0 GeV/c.
description: RHIC-BNL. We report on the first measurement of the charmed-strange meson
DOI: 10.17182/hepdata.101172.v1/t3
title: "Figure 1b (10-40%)" of "Observation of $D_{s}^{\pm}/D^0$ enhancement in Au+Au collisions at $\sqrt{s_{_{NN}}}$ = 200 GeV"

description: $D_s^{\pm}$ invariant yield as a function of $p_{T}$ in 10-40% centrality bin of Au+Au collisions at $\sqrt{s_{_{\rm NN}}}$ = 200 GeV. The $p_T$ bins are 1.0 &lt; $p_T$ &lt; 2.0 GeV/c, 2.0 &lt; $p_T$ &lt; 2.5 GeV/c, 2.5 &lt; $p_T$ &lt; 3.5 GeV/c, 3.5 &lt; $p_T$ &lt; 5.0 GeV/c and 5.0 &lt; $p_T$ &lt; 8.0 GeV/c.
description: RHIC-BNL. We report on the first measurement of the charmed-strange meson
DOI: 10.17182/hepdata.101172.v1/t4
title: "Figure 1b (40-80%)" of "Observation of $D_{s}^{\pm}/D^0$ enhancement in Au+Au collisions at $\sqrt{s_{_{NN}}}$ = 200 GeV"

description: $D_s^{\pm}$ invariant yield as a function of $p_{T}$ in 40-80% centrality bin of Au+Au collisions at $\sqrt{s_{_{\rm NN}}}$ = 200 GeV. The $p_T$ bins are 1.5 &lt; $p_T$ &lt; 2.5 GeV/c, 2.5 &lt; $p_T$ &lt; 3.5 GeV/c, 3.5 &lt; $p_T$ &lt; 5.0 GeV/c and 5.0 &lt; $p_T$ &lt; 8.0 GeV/c.
description: RHIC-BNL. We report on the first measurement of the charmed-strange meson
DOI: 10.17182/hepdata.101172.v1/t10
title: "Figure 4" of "Observation of $D_{s}^{\pm}/D^0$ enhancement in Au+Au collisions at $\sqrt{s_{_{NN}}}$ = 200 GeV"

description: The integrated $D_{s}/D^{0}$ yield ratio within 1.5 &lt; $p_{T}$ &lt; 5.0 GeV/c as a function of collision centrality. The centrality bins are 60-80%, 40-60%, 20-40%, 10-20% and 0-10%.
description: RHIC-BNL. We report on the first measurement of the charmed-strange meson
DOI: 10.17182/hepdata.101172.v1/t5
title: "Figure 2a (0-10%)" of "Observation of $D_{s}^{\pm}/D^0$ enhancement in Au+Au collisions at $\sqrt{s_{_{NN}}}$ = 200 GeV"

description: $D_{s}/D^{0}$ yield ratio as a function of $p_{T}$ in 0-10% centrality bin of Au+Au collisions at $\sqrt{s_{_{\rm NN}}}$ = 200 GeV. The $p_T$ bins are 1.5 &lt; $p_T$ &lt; 2.5 GeV/c, 2.5 &lt; $p_T$ &lt; 3.5 GeV/c, 3.5 &lt; $p_T$ &lt; 5.0 GeV/c and 5.0 &lt; $p_T$ &lt; 8.0 GeV/c.
description: RHIC-BNL. We report on the first measurement of the charmed-strange meson
DOI: 10.17182/hepdata.101172.v1/t6
title: "Figure 2a (10-40%)" of "Observation of $D_{s}^{\pm}/D^0$ enhancement in Au+Au collisions at $\sqrt{s_{_{NN}}}$ = 200 GeV"

description: $D_{s}/D^{0}$ yield ratio as a function of $p_{T}$ in 10-40% centrality bin of Au+Au collisions at $\sqrt{s_{_{\rm NN}}}$ = 200 GeV. The $p_T$ bins are 1.0 &lt; $p_T$ &lt; 2.0 GeV/c, 2.0 &lt; $p_T$ &lt; 2.5 GeV/c, 2.5 &lt; $p_T$ &lt; 3.5 GeV/c, 3.5 &lt; $p_T$ &lt; 5.0 GeV/c and 5.0 &lt; $p_T$ &lt; 8.0 GeV/c.
description: RHIC-BNL. We report on the first measurement of the charmed-strange meson
DOI: 10.17182/hepdata.101172.v1/t7
title: "Figure 2a (40-80%)" of "Observation of $D_{s}^{\pm}/D^0$ enhancement in Au+Au collisions at $\sqrt{s_{_{NN}}}$ = 200 GeV"

description: $D_{s}/D^{0}$ yield ratio as a function of $p_{T}$ in 40-80% centrality bin of Au+Au collisions at $\sqrt{s_{_{\rm NN}}}$ = 200 GeV. The $p_T$ bins are 1.5 &lt; $p_T$ &lt; 2.5 GeV/c, 2.5 &lt; $p_T$ &lt; 3.5 GeV/c, 3.5 &lt; $p_T$ &lt; 5.0 GeV/c and 5.0 &lt; $p_T$ &lt; 8.0 GeV/c.
description: RHIC-BNL. We report on the first measurement of the charmed-strange meson
DOI: 10.17182/hepdata.101172.v1/t8
title: "Figure 3a (10-20%)" of "Observation of $D_{s}^{\pm}/D^0$ enhancement in Au+Au collisions at $\sqrt{s_{_{NN}}}$ = 200 GeV"

description: $D_{s}/D^{0}$ yield ratio as a function of $p_{T}$ in 10-20% centrality bin of Au+Au collisions at $\sqrt{s_{_{\rm NN}}}$ = 200 GeV. The $p_T$ bins are 1.5 &lt; $p_T$ &lt; 2.5 GeV/c, 2.5 &lt; $p_T$ &lt; 3.5 GeV/c, 3.5 &lt; $p_T$ &lt; 5.0 GeV/c and 5.0 &lt; $p_T$ &lt; 8.0 GeV/c.
description: RHIC-BNL. We report on the first measurement of the charmed-strange meson
DOI: 10.17182/hepdata.101172.v1/t9
title: "Figure 3b (20-40%)" of "Observation of $D_{s}^{\pm}/D^0$ enhancement in Au+Au collisions at $\sqrt{s_{_{NN}}}$ = 200 GeV"

description: $D_{s}/D^{0}$ yield ratio as a function of $p_{T}$ in 20-40% centrality bin of Au+Au collisions at $\sqrt{s_{_{\rm NN}}}$ = 200 GeV. The $p_T$ bins are 1.5 &lt; $p_T$ &lt; 2.5 GeV/c, 2.5 &lt; $p_T$ &lt; 3.5 GeV/c, 3.5 &lt; $p_T$ &lt; 5.0 GeV/c and 5.0 &lt; $p_T$ &lt; 8.0 GeV/c.
description: RHIC-BNL. We report on the first measurement of the charmed-strange meson