cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.105720.v1/t20
title: "Supplemental Figure 1 p10pbar40_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/t21
title: "Supplemental Figure 1 p10pbar40_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/t22
title: "Supplemental Figure 1 p20pbar5_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/t23
title: "Supplemental Figure 1 p20pbar5_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/t24
title: "Supplemental Figure 1 p20pbar10_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/t25
title: "Supplemental Figure 1 p20pbar10_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/t26
title: "Supplemental Figure 1 p20pbar20_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/t27
title: "Supplemental Figure 1 p20pbar20_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/t28
title: "Supplemental Figure 1 p20pbar40_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/t29
title: "Supplemental Figure 1 p20pbar40_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/t30
title: "Supplemental Figure 1 p40pbar5_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/t31
title: "Supplemental Figure 1 p40pbar5_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/t32
title: "Supplemental Figure 1 p40pbar10_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: 10.25549/vercoutere-ouc110610996
title: 3 military war planes

description: Three military war planes outlined in blue, one labeled x-3, one e-724, and the other indistinguishable. Includes the words: Miliatary War Planes. See 143~02 for possible magazine photo used as inspiration for drawing.
DOI: 10.17182/hepdata.105720.v1/t33
title: "Supplemental Figure 1 p40pbar10_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.