cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.105720.v1/t7
title: "Figure 2, 27 GeV rapidity dependence" of "Measurement of the sixth-order cumulant of net-proton multiplicity distributions in Au+Au collisions at $\sqrt{s_{NN}}=$ 27, 54.4, and 200 GeV at RHIC"

description: Net-proton $C_{6}/C_{2}$ as a function of rapidity (left) and transverse momentum acceptance (right) from $\sqrt{s_{NN}}$ = 27 GeV (crosses), 54.4 (open squares), and 200 GeV (filled circles) Au+Au collisions. The upper and lower plots are for 0-10% and 30-40% centralities, respectively. The error bars are statistical and caps are systematic errors. Points for different beam energies are staggered horizontally to improve clarity. UrQMD transport model results are shown as shaded and hatched bands. The Skellam expectation ($C_{6}/C_{2} = 1) is shown as long-dashed lines.
description: According to the first principle Lattice QCD calculations, the transition from quark-gluon plasma to hadronic matter is a smooth crossover in the region $\mu_{B}$ ≤ $T_{c}$. As a result, higher-order cumulants and their ratios are predicted to be negative, $C_{6}/C_{2}$ &lt; 0, for example. In this paper, we report the first measurement of the midrapidity net-proton $C_{6}/C_{2}$ from 27, 54.4 and 200 GeV Au+Au collisions at RHIC. The dependence on collision centrality and kinematic acceptance in ($p_{T}$ , $y$) are analyzed. While for 54.4 GeV collisions, most of C6/C2 values are larger or equal to zero, it is observed that for 27 and 200 GeV collisions, the values of C6/C2 progressively become negative from peripheral to central collisions. Transport model calculations without critical dynamics predict values around zero. These observations seem in favor of a smooth crossover in the high energy nuclear collisions at RHIC.
DOI: 10.17182/hepdata.105720.v1/t8
title: "Figure 2, 27 GeV $p_{T}$ dependence" of "Measurement of the sixth-order cumulant of net-proton multiplicity distributions in Au+Au collisions at $\sqrt{s_{NN}}=$ 27, 54.4, and 200 GeV at RHIC"

description: Net-proton $C_{6}/C_{2}$ as a function of rapidity (left) and transverse momentum acceptance (right) from $\sqrt{s_{NN}}$ = 27 GeV (crosses), 54.4 (open squares), and 200 GeV (filled circles) Au+Au collisions. The upper and lower plots are for 0-10% and 30-40% centralities, respectively. The error bars are statistical and caps are systematic errors. Points for different beam energies are staggered horizontally to improve clarity. UrQMD transport model results are shown as shaded and hatched bands. The Skellam expectation ($C_{6}/C_{2} = 1) is shown as long-dashed lines.
description: According to the first principle Lattice QCD calculations, the transition from quark-gluon plasma to hadronic matter is a smooth crossover in the region $\mu_{B}$ ≤ $T_{c}$. As a result, higher-order cumulants and their ratios are predicted to be negative, $C_{6}/C_{2}$ &lt; 0, for example. In this paper, we report the first measurement of the midrapidity net-proton $C_{6}/C_{2}$ from 27, 54.4 and 200 GeV Au+Au collisions at RHIC. The dependence on collision centrality and kinematic acceptance in ($p_{T}$ , $y$) are analyzed. While for 54.4 GeV collisions, most of C6/C2 values are larger or equal to zero, it is observed that for 27 and 200 GeV collisions, the values of C6/C2 progressively become negative from peripheral to central collisions. Transport model calculations without critical dynamics predict values around zero. These observations seem in favor of a smooth crossover in the high energy nuclear collisions at RHIC.
DOI: 10.17182/hepdata.105720.v1/t9
title: "Figure 2, 54.4 GeV rapidity dependence" of "Measurement of the sixth-order cumulant of net-proton multiplicity distributions in Au+Au collisions at $\sqrt{s_{NN}}=$ 27, 54.4, and 200 GeV at RHIC"

description: Net-proton $C_{6}/C_{2}$ as a function of rapidity (left) and transverse momentum acceptance (right) from $\sqrt{s_{NN}}$ = 27 GeV (crosses), 54.4 (open squares), and 200 GeV (filled circles) Au+Au collisions. The upper and lower plots are for 0-10% and 30-40% centralities, respectively. The error bars are statistical and caps are systematic errors. Points for different beam energies are staggered horizontally to improve clarity. UrQMD transport model results are shown as shaded and hatched bands. The Skellam expectation ($C_{6}/C_{2} = 1) is shown as long-dashed lines.
description: According to the first principle Lattice QCD calculations, the transition from quark-gluon plasma to hadronic matter is a smooth crossover in the region $\mu_{B}$ ≤ $T_{c}$. As a result, higher-order cumulants and their ratios are predicted to be negative, $C_{6}/C_{2}$ &lt; 0, for example. In this paper, we report the first measurement of the midrapidity net-proton $C_{6}/C_{2}$ from 27, 54.4 and 200 GeV Au+Au collisions at RHIC. The dependence on collision centrality and kinematic acceptance in ($p_{T}$ , $y$) are analyzed. While for 54.4 GeV collisions, most of C6/C2 values are larger or equal to zero, it is observed that for 27 and 200 GeV collisions, the values of C6/C2 progressively become negative from peripheral to central collisions. Transport model calculations without critical dynamics predict values around zero. These observations seem in favor of a smooth crossover in the high energy nuclear collisions at RHIC.
DOI: 10.25549/vercoutere-ouc110610986
title: Bridge

description: Bridge with wood sides and supporting arches with sky above, includes a header with the word: Bridge. Words on the reverse side written by OT: Patient went to sleep after doing this altho usually active in the yard
DOI: 10.17182/hepdata.105720.v1/t10
title: "Figure 2, 54.4 GeV $p_{T}$ dependence" of "Measurement of the sixth-order cumulant of net-proton multiplicity distributions in Au+Au collisions at $\sqrt{s_{NN}}=$ 27, 54.4, and 200 GeV at RHIC"

description: Net-proton $C_{6}/C_{2}$ as a function of rapidity (left) and transverse momentum acceptance (right) from $\sqrt{s_{NN}}$ = 27 GeV (crosses), 54.4 (open squares), and 200 GeV (filled circles) Au+Au collisions. The upper and lower plots are for 0-10% and 30-40% centralities, respectively. The error bars are statistical and caps are systematic errors. Points for different beam energies are staggered horizontally to improve clarity. UrQMD transport model results are shown as shaded and hatched bands. The Skellam expectation ($C_{6}/C_{2} = 1) is shown as long-dashed lines.
description: According to the first principle Lattice QCD calculations, the transition from quark-gluon plasma to hadronic matter is a smooth crossover in the region $\mu_{B}$ ≤ $T_{c}$. As a result, higher-order cumulants and their ratios are predicted to be negative, $C_{6}/C_{2}$ &lt; 0, for example. In this paper, we report the first measurement of the midrapidity net-proton $C_{6}/C_{2}$ from 27, 54.4 and 200 GeV Au+Au collisions at RHIC. The dependence on collision centrality and kinematic acceptance in ($p_{T}$ , $y$) are analyzed. While for 54.4 GeV collisions, most of C6/C2 values are larger or equal to zero, it is observed that for 27 and 200 GeV collisions, the values of C6/C2 progressively become negative from peripheral to central collisions. Transport model calculations without critical dynamics predict values around zero. These observations seem in favor of a smooth crossover in the high energy nuclear collisions at RHIC.
DOI: 10.17182/hepdata.105720.v1/t11
title: "Figure 2, 200 GeV rapidity dependence" of "Measurement of the sixth-order cumulant of net-proton multiplicity distributions in Au+Au collisions at $\sqrt{s_{NN}}=$ 27, 54.4, and 200 GeV at RHIC"

description: Net-proton $C_{6}/C_{2}$ as a function of rapidity (left) and transverse momentum acceptance (right) from $\sqrt{s_{NN}}$ = 27 GeV (crosses), 54.4 (open squares), and 200 GeV (filled circles) Au+Au collisions. The upper and lower plots are for 0-10% and 30-40% centralities, respectively. The error bars are statistical and caps are systematic errors. Points for different beam energies are staggered horizontally to improve clarity. UrQMD transport model results are shown as shaded and hatched bands. The Skellam expectation ($C_{6}/C_{2} = 1) is shown as long-dashed lines.
description: According to the first principle Lattice QCD calculations, the transition from quark-gluon plasma to hadronic matter is a smooth crossover in the region $\mu_{B}$ ≤ $T_{c}$. As a result, higher-order cumulants and their ratios are predicted to be negative, $C_{6}/C_{2}$ &lt; 0, for example. In this paper, we report the first measurement of the midrapidity net-proton $C_{6}/C_{2}$ from 27, 54.4 and 200 GeV Au+Au collisions at RHIC. The dependence on collision centrality and kinematic acceptance in ($p_{T}$ , $y$) are analyzed. While for 54.4 GeV collisions, most of C6/C2 values are larger or equal to zero, it is observed that for 27 and 200 GeV collisions, the values of C6/C2 progressively become negative from peripheral to central collisions. Transport model calculations without critical dynamics predict values around zero. These observations seem in favor of a smooth crossover in the high energy nuclear collisions at RHIC.
DOI: 10.17182/hepdata.105720.v1/t12
title: "Figure 2, 200 GeV $p_{T}$ dependence" of "Measurement of the sixth-order cumulant of net-proton multiplicity distributions in Au+Au collisions at $\sqrt{s_{NN}}=$ 27, 54.4, and 200 GeV at RHIC"

description: Net-proton $C_{6}/C_{2}$ as a function of rapidity (left) and transverse momentum acceptance (right) from $\sqrt{s_{NN}}$ = 27 GeV (crosses), 54.4 (open squares), and 200 GeV (filled circles) Au+Au collisions. The upper and lower plots are for 0-10% and 30-40% centralities, respectively. The error bars are statistical and caps are systematic errors. Points for different beam energies are staggered horizontally to improve clarity. UrQMD transport model results are shown as shaded and hatched bands. The Skellam expectation ($C_{6}/C_{2} = 1) is shown as long-dashed lines.
description: According to the first principle Lattice QCD calculations, the transition from quark-gluon plasma to hadronic matter is a smooth crossover in the region $\mu_{B}$ ≤ $T_{c}$. As a result, higher-order cumulants and their ratios are predicted to be negative, $C_{6}/C_{2}$ &lt; 0, for example. In this paper, we report the first measurement of the midrapidity net-proton $C_{6}/C_{2}$ from 27, 54.4 and 200 GeV Au+Au collisions at RHIC. The dependence on collision centrality and kinematic acceptance in ($p_{T}$ , $y$) are analyzed. While for 54.4 GeV collisions, most of C6/C2 values are larger or equal to zero, it is observed that for 27 and 200 GeV collisions, the values of C6/C2 progressively become negative from peripheral to central collisions. Transport model calculations without critical dynamics predict values around zero. These observations seem in favor of a smooth crossover in the high energy nuclear collisions at RHIC.
DOI: 10.17182/hepdata.105720.v1/t13
title: "Figure 3, 27 GeV" of "Measurement of the sixth-order cumulant of net-proton multiplicity distributions in Au+Au collisions at $\sqrt{s_{NN}}=$ 27, 54.4, and 200 GeV at RHIC"

description: Collisions centrality dependence of net-proton $C_{6}/C_{2}$ in Au+Au collisions for |$y$| &lt; 0.5 and 0.4 &lt; $p_{T}$ (GeV/c) &lt; 2.0. The error bars are statistical and caps are systematic errors. Points for different beam energies are staggered horizontally to improve clarity. A shaded band shows the results from UrQMD model calculations. UrQMD calculations from the above three collision energies are consistent among them so they are merged in order to reduce statistical fluctuations. Details on these calculations can be found in the Supplemental Material at [URL will be inserted by publisher]. The lattice QCD calculations [16, 17] for T = 160 MeV and $\mu_{B}$ &lt; 110 MeV. are shown as a blue band at $\langle N_{part}\rangle$ $\approx$ 340.
description: According to the first principle Lattice QCD calculations, the transition from quark-gluon plasma to hadronic matter is a smooth crossover in the region $\mu_{B}$ ≤ $T_{c}$. As a result, higher-order cumulants and their ratios are predicted to be negative, $C_{6}/C_{2}$ &lt; 0, for example. In this paper, we report the first measurement of the midrapidity net-proton $C_{6}/C_{2}$ from 27, 54.4 and 200 GeV Au+Au collisions at RHIC. The dependence on collision centrality and kinematic acceptance in ($p_{T}$ , $y$) are analyzed. While for 54.4 GeV collisions, most of C6/C2 values are larger or equal to zero, it is observed that for 27 and 200 GeV collisions, the values of C6/C2 progressively become negative from peripheral to central collisions. Transport model calculations without critical dynamics predict values around zero. These observations seem in favor of a smooth crossover in the high energy nuclear collisions at RHIC.
DOI: 10.17182/hepdata.105720.v1/t14
title: "Figure 3, 54.4 GeV" of "Measurement of the sixth-order cumulant of net-proton multiplicity distributions in Au+Au collisions at $\sqrt{s_{NN}}=$ 27, 54.4, and 200 GeV at RHIC"

description: Collisions centrality dependence of net-proton $C_{6}/C_{2}$ in Au+Au collisions for |$y$| &lt; 0.5 and 0.4 &lt; $p_{T}$ (GeV/c) &lt; 2.0. The error bars are statistical and caps are systematic errors. Points for different beam energies are staggered horizontally to improve clarity. A shaded band shows the results from UrQMD model calculations. UrQMD calculations from the above three collision energies are consistent among them so they are merged in order to reduce statistical fluctuations. Details on these calculations can be found in the Supplemental Material at [URL will be inserted by publisher]. The lattice QCD calculations [16, 17] for T = 160 MeV and $\mu_{B}$ &lt; 110 MeV. are shown as a blue band at $\langle N_{part}\rangle$ $\approx$ 340.
description: According to the first principle Lattice QCD calculations, the transition from quark-gluon plasma to hadronic matter is a smooth crossover in the region $\mu_{B}$ ≤ $T_{c}$. As a result, higher-order cumulants and their ratios are predicted to be negative, $C_{6}/C_{2}$ &lt; 0, for example. In this paper, we report the first measurement of the midrapidity net-proton $C_{6}/C_{2}$ from 27, 54.4 and 200 GeV Au+Au collisions at RHIC. The dependence on collision centrality and kinematic acceptance in ($p_{T}$ , $y$) are analyzed. While for 54.4 GeV collisions, most of C6/C2 values are larger or equal to zero, it is observed that for 27 and 200 GeV collisions, the values of C6/C2 progressively become negative from peripheral to central collisions. Transport model calculations without critical dynamics predict values around zero. These observations seem in favor of a smooth crossover in the high energy nuclear collisions at RHIC.
DOI: 10.17182/hepdata.105720.v1/t15
title: "Figure 3, 200 GeV" of "Measurement of the sixth-order cumulant of net-proton multiplicity distributions in Au+Au collisions at $\sqrt{s_{NN}}=$ 27, 54.4, and 200 GeV at RHIC"

description: Collisions centrality dependence of net-proton $C_{6}/C_{2}$ in Au+Au collisions for |$y$| &lt; 0.5 and 0.4 &lt; $p_{T}$ (GeV/c) &lt; 2.0. The error bars are statistical and caps are systematic errors. Points for different beam energies are staggered horizontally to improve clarity. A shaded band shows the results from UrQMD model calculations. UrQMD calculations from the above three collision energies are consistent among them so they are merged in order to reduce statistical fluctuations. Details on these calculations can be found in the Supplemental Material at [URL will be inserted by publisher]. The lattice QCD calculations [16, 17] for T = 160 MeV and $\mu_{B}$ &lt; 110 MeV. are shown as a blue band at $\langle N_{part}\rangle$ $\approx$ 340.
description: According to the first principle Lattice QCD calculations, the transition from quark-gluon plasma to hadronic matter is a smooth crossover in the region $\mu_{B}$ ≤ $T_{c}$. As a result, higher-order cumulants and their ratios are predicted to be negative, $C_{6}/C_{2}$ &lt; 0, for example. In this paper, we report the first measurement of the midrapidity net-proton $C_{6}/C_{2}$ from 27, 54.4 and 200 GeV Au+Au collisions at RHIC. The dependence on collision centrality and kinematic acceptance in ($p_{T}$ , $y$) are analyzed. While for 54.4 GeV collisions, most of C6/C2 values are larger or equal to zero, it is observed that for 27 and 200 GeV collisions, the values of C6/C2 progressively become negative from peripheral to central collisions. Transport model calculations without critical dynamics predict values around zero. These observations seem in favor of a smooth crossover in the high energy nuclear collisions at RHIC.
DOI: 10.17182/hepdata.105720.v1/t16
title: "Supplemental Figure 1 p10pbar10_Beta_Binomial, 200 GeV" of "Measurement of the sixth-order cumulant of net-proton multiplicity distributions in Au+Au collisions at $\sqrt{s_{NN}}=$ 27, 54.4, and 200 GeV at RHIC"

description: Distributions of reconstructed protons (black circles) from embedding simulations in 200 GeV Au+Au collisions at 0-2.5% centrality. Red lines are fits with the binomial distribution, and green dotted lines represent the fit with the beta-binomial distributions using α that gives the minimal chi2/ndf. Each panel shows the result from the given combinations of embedded protons and antiprotons. The ratio of fits to the embedding data is shown for each panel.
description: According to the first principle Lattice QCD calculations, the transition from quark-gluon plasma to hadronic matter is a smooth crossover in the region $\mu_{B}$ ≤ $T_{c}$. As a result, higher-order cumulants and their ratios are predicted to be negative, $C_{6}/C_{2}$ &lt; 0, for example. In this paper, we report the first measurement of the midrapidity net-proton $C_{6}/C_{2}$ from 27, 54.4 and 200 GeV Au+Au collisions at RHIC. The dependence on collision centrality and kinematic acceptance in ($p_{T}$ , $y$) are analyzed. While for 54.4 GeV collisions, most of C6/C2 values are larger or equal to zero, it is observed that for 27 and 200 GeV collisions, the values of C6/C2 progressively become negative from peripheral to central collisions. Transport model calculations without critical dynamics predict values around zero. These observations seem in favor of a smooth crossover in the high energy nuclear collisions at RHIC.
DOI: 10.17182/hepdata.105720.v1/t17
title: "Supplemental Figure 1 p10pbar10_embedding, 200 GeV" of "Measurement of the sixth-order cumulant of net-proton multiplicity distributions in Au+Au collisions at $\sqrt{s_{NN}}=$ 27, 54.4, and 200 GeV at RHIC"

description: Distributions of reconstructed protons (black circles) from embedding simulations in 200 GeV Au+Au collisions at 0-2.5% centrality. Red lines are fits with the binomial distribution, and green dotted lines represent the fit with the beta-binomial distributions using α that gives the minimal chi2/ndf. Each panel shows the result from the given combinations of embedded protons and antiprotons. The ratio of fits to the embedding data is shown for each panel.
description: According to the first principle Lattice QCD calculations, the transition from quark-gluon plasma to hadronic matter is a smooth crossover in the region $\mu_{B}$ ≤ $T_{c}$. As a result, higher-order cumulants and their ratios are predicted to be negative, $C_{6}/C_{2}$ &lt; 0, for example. In this paper, we report the first measurement of the midrapidity net-proton $C_{6}/C_{2}$ from 27, 54.4 and 200 GeV Au+Au collisions at RHIC. The dependence on collision centrality and kinematic acceptance in ($p_{T}$ , $y$) are analyzed. While for 54.4 GeV collisions, most of C6/C2 values are larger or equal to zero, it is observed that for 27 and 200 GeV collisions, the values of C6/C2 progressively become negative from peripheral to central collisions. Transport model calculations without critical dynamics predict values around zero. These observations seem in favor of a smooth crossover in the high energy nuclear collisions at RHIC.
DOI: 10.17182/hepdata.105720.v1/t18
title: "Supplemental Figure 1 p10pbar20_Beta_Binomial, 200 GeV" of "Measurement of the sixth-order cumulant of net-proton multiplicity distributions in Au+Au collisions at $\sqrt{s_{NN}}=$ 27, 54.4, and 200 GeV at RHIC"

description: Distributions of reconstructed protons (black circles) from embedding simulations in 200 GeV Au+Au collisions at 0-2.5% centrality. Red lines are fits with the binomial distribution, and green dotted lines represent the fit with the beta-binomial distributions using α that gives the minimal chi2/ndf. Each panel shows the result from the given combinations of embedded protons and antiprotons. The ratio of fits to the embedding data is shown for each panel.
description: According to the first principle Lattice QCD calculations, the transition from quark-gluon plasma to hadronic matter is a smooth crossover in the region $\mu_{B}$ ≤ $T_{c}$. As a result, higher-order cumulants and their ratios are predicted to be negative, $C_{6}/C_{2}$ &lt; 0, for example. In this paper, we report the first measurement of the midrapidity net-proton $C_{6}/C_{2}$ from 27, 54.4 and 200 GeV Au+Au collisions at RHIC. The dependence on collision centrality and kinematic acceptance in ($p_{T}$ , $y$) are analyzed. While for 54.4 GeV collisions, most of C6/C2 values are larger or equal to zero, it is observed that for 27 and 200 GeV collisions, the values of C6/C2 progressively become negative from peripheral to central collisions. Transport model calculations without critical dynamics predict values around zero. These observations seem in favor of a smooth crossover in the high energy nuclear collisions at RHIC.
DOI: 10.17182/hepdata.105720.v1/t19
title: "Supplemental Figure 1 p10pbar20_embedding, 200 GeV" of "Measurement of the sixth-order cumulant of net-proton multiplicity distributions in Au+Au collisions at $\sqrt{s_{NN}}=$ 27, 54.4, and 200 GeV at RHIC"

description: Distributions of reconstructed protons (black circles) from embedding simulations in 200 GeV Au+Au collisions at 0-2.5% centrality. Red lines are fits with the binomial distribution, and green dotted lines represent the fit with the beta-binomial distributions using α that gives the minimal chi2/ndf. Each panel shows the result from the given combinations of embedded protons and antiprotons. The ratio of fits to the embedding data is shown for each panel.
description: According to the first principle Lattice QCD calculations, the transition from quark-gluon plasma to hadronic matter is a smooth crossover in the region $\mu_{B}$ ≤ $T_{c}$. As a result, higher-order cumulants and their ratios are predicted to be negative, $C_{6}/C_{2}$ &lt; 0, for example. In this paper, we report the first measurement of the midrapidity net-proton $C_{6}/C_{2}$ from 27, 54.4 and 200 GeV Au+Au collisions at RHIC. The dependence on collision centrality and kinematic acceptance in ($p_{T}$ , $y$) are analyzed. While for 54.4 GeV collisions, most of C6/C2 values are larger or equal to zero, it is observed that for 27 and 200 GeV collisions, the values of C6/C2 progressively become negative from peripheral to central collisions. Transport model calculations without critical dynamics predict values around zero. These observations seem in favor of a smooth crossover in the high energy nuclear collisions at RHIC.