cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.96906.v1/t20
title: "Figure 7d ($\Xi^{-}+\bar{\Xi}^{+}$)" of "Centrality dependence of charged hadron and strange hadron elliptic flow from sqrt(s_NN) = 200 GeV Au+Au collisions"

description: $v_{2}$ of $\Xi^{-}+\bar{\Xi}^{+}$ (filled triangles) as a function of $p_{T}$ for (d) $0–10\%$ centrality in $Au+Au$ collisions at $\sqrt{s_{NN}} = 200$ GeV.
description: We present STAR results on the elliptic flow $v_2$ of charged hadrons, strange and multi-strange particles from $\sqrt{s_{NN}} = 200$ GeV $Au+Au$ collisions at RHIC. The detailed study of the centrality dependence of $v_{2}$ over a broad transverse momentum range is presented. Comparison of different analysis methods are made in order to estimate systematic uncertainties. In order to discuss the non-flow effect, we have performed the first analysis of $v_{2}$ with the Lee-Yang Zero method for $K_{S}^{0}$ and $\Lambda$. In the relatively low $p_{T}$ region, $p_{T} \le 2$ GeV/c, a scaling with $m_{T}−m$ is observed for identified hadrons in each centrality bin studied. However, we do not observe $v_{2}(p_{T})$ scaled by the participant eccentricity to be independent of centrality. At higher $p_{T}$ , $2 \le p_{T} \le 6$ GeV/c, $v_{2}$ scales 3 with quark number for all hadrons studied. For the multi-strange hadron $\Omega$, which does not suffer appreciable hadronic interactions, the values of $v_{2}$ are consistent with both $m_{T}−m$ scaling at low $p_{T}$ and number-of-quark scaling at intermediate $p_{T}$. As a function of collision centrality, an increase of $p_{T}$-integrated $v_{2}$ scaled by the participant eccentricity has been observed, indicating a stronger collective flow in more central $Au+Au$ collisions.
DOI: 10.17182/hepdata.96906.v1/t21
title: "Figure 7a ($\Omega^{-}+\bar{\Omega}^{+}$)" of "Centrality dependence of charged hadron and strange hadron elliptic flow from sqrt(s_NN) = 200 GeV Au+Au collisions"

description: $v_{2}$ of $\Omega^{-}+\bar{\Omega}^{+}$ (filled circles) as a function of $p_{T}$ for (a) $0–80\%$ centrality in $Au+Au$ collisions at $\sqrt{s_{NN}} = 200$ GeV.
description: We present STAR results on the elliptic flow $v_2$ of charged hadrons, strange and multi-strange particles from $\sqrt{s_{NN}} = 200$ GeV $Au+Au$ collisions at RHIC. The detailed study of the centrality dependence of $v_{2}$ over a broad transverse momentum range is presented. Comparison of different analysis methods are made in order to estimate systematic uncertainties. In order to discuss the non-flow effect, we have performed the first analysis of $v_{2}$ with the Lee-Yang Zero method for $K_{S}^{0}$ and $\Lambda$. In the relatively low $p_{T}$ region, $p_{T} \le 2$ GeV/c, a scaling with $m_{T}−m$ is observed for identified hadrons in each centrality bin studied. However, we do not observe $v_{2}(p_{T})$ scaled by the participant eccentricity to be independent of centrality. At higher $p_{T}$ , $2 \le p_{T} \le 6$ GeV/c, $v_{2}$ scales 3 with quark number for all hadrons studied. For the multi-strange hadron $\Omega$, which does not suffer appreciable hadronic interactions, the values of $v_{2}$ are consistent with both $m_{T}−m$ scaling at low $p_{T}$ and number-of-quark scaling at intermediate $p_{T}$. As a function of collision centrality, an increase of $p_{T}$-integrated $v_{2}$ scaled by the participant eccentricity has been observed, indicating a stronger collective flow in more central $Au+Au$ collisions.
DOI: 10.17182/hepdata.96906.v1/t22
title: "Figure 7d ($\Omega^{-}+\bar{\Omega}^{+}$)" of "Centrality dependence of charged hadron and strange hadron elliptic flow from sqrt(s_NN) = 200 GeV Au+Au collisions"

description: $v_{2}$ of $\Omega^{-}+\bar{\Omega}^{+}$ (filled circles) as a function of $p_{T}$ for (d) $0–10\%$ centrality in $Au+Au$ collisions at $\sqrt{s_{NN}} = 200$ GeV.
description: We present STAR results on the elliptic flow $v_2$ of charged hadrons, strange and multi-strange particles from $\sqrt{s_{NN}} = 200$ GeV $Au+Au$ collisions at RHIC. The detailed study of the centrality dependence of $v_{2}$ over a broad transverse momentum range is presented. Comparison of different analysis methods are made in order to estimate systematic uncertainties. In order to discuss the non-flow effect, we have performed the first analysis of $v_{2}$ with the Lee-Yang Zero method for $K_{S}^{0}$ and $\Lambda$. In the relatively low $p_{T}$ region, $p_{T} \le 2$ GeV/c, a scaling with $m_{T}−m$ is observed for identified hadrons in each centrality bin studied. However, we do not observe $v_{2}(p_{T})$ scaled by the participant eccentricity to be independent of centrality. At higher $p_{T}$ , $2 \le p_{T} \le 6$ GeV/c, $v_{2}$ scales 3 with quark number for all hadrons studied. For the multi-strange hadron $\Omega$, which does not suffer appreciable hadronic interactions, the values of $v_{2}$ are consistent with both $m_{T}−m$ scaling at low $p_{T}$ and number-of-quark scaling at intermediate $p_{T}$. As a function of collision centrality, an increase of $p_{T}$-integrated $v_{2}$ scaled by the participant eccentricity has been observed, indicating a stronger collective flow in more central $Au+Au$ collisions.
DOI: 10.17182/hepdata.96906.v1/t23
title: "Figure 7a ($p+\bar{p}$ and $\pi^{+}+\pi^{-}$)" of "Centrality dependence of charged hadron and strange hadron elliptic flow from sqrt(s_NN) = 200 GeV Au+Au collisions"

description: $v_{2}$ of $p+\bar{p}$ (filled squares) and $\pi^{+}+\pi^{-}$ (filled stars) as a function of $p_{T}$ for (a) $0–80\%$ centrality in $Au+Au$ collisions at $\sqrt{s_{NN}} = 200$ GeV.
description: We present STAR results on the elliptic flow $v_2$ of charged hadrons, strange and multi-strange particles from $\sqrt{s_{NN}} = 200$ GeV $Au+Au$ collisions at RHIC. The detailed study of the centrality dependence of $v_{2}$ over a broad transverse momentum range is presented. Comparison of different analysis methods are made in order to estimate systematic uncertainties. In order to discuss the non-flow effect, we have performed the first analysis of $v_{2}$ with the Lee-Yang Zero method for $K_{S}^{0}$ and $\Lambda$. In the relatively low $p_{T}$ region, $p_{T} \le 2$ GeV/c, a scaling with $m_{T}−m$ is observed for identified hadrons in each centrality bin studied. However, we do not observe $v_{2}(p_{T})$ scaled by the participant eccentricity to be independent of centrality. At higher $p_{T}$ , $2 \le p_{T} \le 6$ GeV/c, $v_{2}$ scales 3 with quark number for all hadrons studied. For the multi-strange hadron $\Omega$, which does not suffer appreciable hadronic interactions, the values of $v_{2}$ are consistent with both $m_{T}−m$ scaling at low $p_{T}$ and number-of-quark scaling at intermediate $p_{T}$. As a function of collision centrality, an increase of $p_{T}$-integrated $v_{2}$ scaled by the participant eccentricity has been observed, indicating a stronger collective flow in more central $Au+Au$ collisions.
DOI: 10.17182/hepdata.96906.v1/t24
title: "Figure 12d inset ($\Lambda$)" of "Centrality dependence of charged hadron and strange hadron elliptic flow from sqrt(s_NN) = 200 GeV Au+Au collisions"

description: Fig12d inset $\Lambda$ (open squares) expansion at low $p_{T}$
description: We present STAR results on the elliptic flow $v_2$ of charged hadrons, strange and multi-strange particles from $\sqrt{s_{NN}} = 200$ GeV $Au+Au$ collisions at RHIC. The detailed study of the centrality dependence of $v_{2}$ over a broad transverse momentum range is presented. Comparison of different analysis methods are made in order to estimate systematic uncertainties. In order to discuss the non-flow effect, we have performed the first analysis of $v_{2}$ with the Lee-Yang Zero method for $K_{S}^{0}$ and $\Lambda$. In the relatively low $p_{T}$ region, $p_{T} \le 2$ GeV/c, a scaling with $m_{T}−m$ is observed for identified hadrons in each centrality bin studied. However, we do not observe $v_{2}(p_{T})$ scaled by the participant eccentricity to be independent of centrality. At higher $p_{T}$ , $2 \le p_{T} \le 6$ GeV/c, $v_{2}$ scales 3 with quark number for all hadrons studied. For the multi-strange hadron $\Omega$, which does not suffer appreciable hadronic interactions, the values of $v_{2}$ are consistent with both $m_{T}−m$ scaling at low $p_{T}$ and number-of-quark scaling at intermediate $p_{T}$. As a function of collision centrality, an increase of $p_{T}$-integrated $v_{2}$ scaled by the participant eccentricity has been observed, indicating a stronger collective flow in more central $Au+Au$ collisions.
DOI: 10.17182/hepdata.96906.v1/t25
title: "Figure 12d inset ($K_{S}^{0}$)" of "Centrality dependence of charged hadron and strange hadron elliptic flow from sqrt(s_NN) = 200 GeV Au+Au collisions"

description: Fig12d inset for $K_{S}^{0}$ (filled circles) expansion at low $p_{T}$
description: We present STAR results on the elliptic flow $v_2$ of charged hadrons, strange and multi-strange particles from $\sqrt{s_{NN}} = 200$ GeV $Au+Au$ collisions at RHIC. The detailed study of the centrality dependence of $v_{2}$ over a broad transverse momentum range is presented. Comparison of different analysis methods are made in order to estimate systematic uncertainties. In order to discuss the non-flow effect, we have performed the first analysis of $v_{2}$ with the Lee-Yang Zero method for $K_{S}^{0}$ and $\Lambda$. In the relatively low $p_{T}$ region, $p_{T} \le 2$ GeV/c, a scaling with $m_{T}−m$ is observed for identified hadrons in each centrality bin studied. However, we do not observe $v_{2}(p_{T})$ scaled by the participant eccentricity to be independent of centrality. At higher $p_{T}$ , $2 \le p_{T} \le 6$ GeV/c, $v_{2}$ scales 3 with quark number for all hadrons studied. For the multi-strange hadron $\Omega$, which does not suffer appreciable hadronic interactions, the values of $v_{2}$ are consistent with both $m_{T}−m$ scaling at low $p_{T}$ and number-of-quark scaling at intermediate $p_{T}$. As a function of collision centrality, an increase of $p_{T}$-integrated $v_{2}$ scaled by the participant eccentricity has been observed, indicating a stronger collective flow in more central $Au+Au$ collisions.
DOI: 10.17182/hepdata.96906.v1/t26
title: "Figure 13 (charged hadrons)" of "Centrality dependence of charged hadron and strange hadron elliptic flow from sqrt(s_NN) = 200 GeV Au+Au collisions"

description: Fig13 Centrality dependence of $v_{2}$ versus number of participants $N_{part}$ for charged hadrons (crosses) in $Au+Au$ collisions at $\sqrt{s_{NN}} = 200$ GeV. For identified particle's value, $v_{2}$ in Tab. II scaled by participant eccentricity in Tab. I versus number of participant in Tab. I.
description: We present STAR results on the elliptic flow $v_2$ of charged hadrons, strange and multi-strange particles from $\sqrt{s_{NN}} = 200$ GeV $Au+Au$ collisions at RHIC. The detailed study of the centrality dependence of $v_{2}$ over a broad transverse momentum range is presented. Comparison of different analysis methods are made in order to estimate systematic uncertainties. In order to discuss the non-flow effect, we have performed the first analysis of $v_{2}$ with the Lee-Yang Zero method for $K_{S}^{0}$ and $\Lambda$. In the relatively low $p_{T}$ region, $p_{T} \le 2$ GeV/c, a scaling with $m_{T}−m$ is observed for identified hadrons in each centrality bin studied. However, we do not observe $v_{2}(p_{T})$ scaled by the participant eccentricity to be independent of centrality. At higher $p_{T}$ , $2 \le p_{T} \le 6$ GeV/c, $v_{2}$ scales 3 with quark number for all hadrons studied. For the multi-strange hadron $\Omega$, which does not suffer appreciable hadronic interactions, the values of $v_{2}$ are consistent with both $m_{T}−m$ scaling at low $p_{T}$ and number-of-quark scaling at intermediate $p_{T}$. As a function of collision centrality, an increase of $p_{T}$-integrated $v_{2}$ scaled by the participant eccentricity has been observed, indicating a stronger collective flow in more central $Au+Au$ collisions.
DOI: 10.17182/hepdata.96906.v1/t27
title: "Figure 14 ($K_{S}^{0}$)" of "Centrality dependence of charged hadron and strange hadron elliptic flow from sqrt(s_NN) = 200 GeV Au+Au collisions"

description: Fig14 $p_{T}$ dependence of $v_{2}$ of $K_{S}^{0}$ at 200 GeV.
description: We present STAR results on the elliptic flow $v_2$ of charged hadrons, strange and multi-strange particles from $\sqrt{s_{NN}} = 200$ GeV $Au+Au$ collisions at RHIC. The detailed study of the centrality dependence of $v_{2}$ over a broad transverse momentum range is presented. Comparison of different analysis methods are made in order to estimate systematic uncertainties. In order to discuss the non-flow effect, we have performed the first analysis of $v_{2}$ with the Lee-Yang Zero method for $K_{S}^{0}$ and $\Lambda$. In the relatively low $p_{T}$ region, $p_{T} \le 2$ GeV/c, a scaling with $m_{T}−m$ is observed for identified hadrons in each centrality bin studied. However, we do not observe $v_{2}(p_{T})$ scaled by the participant eccentricity to be independent of centrality. At higher $p_{T}$ , $2 \le p_{T} \le 6$ GeV/c, $v_{2}$ scales 3 with quark number for all hadrons studied. For the multi-strange hadron $\Omega$, which does not suffer appreciable hadronic interactions, the values of $v_{2}$ are consistent with both $m_{T}−m$ scaling at low $p_{T}$ and number-of-quark scaling at intermediate $p_{T}$. As a function of collision centrality, an increase of $p_{T}$-integrated $v_{2}$ scaled by the participant eccentricity has been observed, indicating a stronger collective flow in more central $Au+Au$ collisions.
DOI: 10.3535/asl-rvd-g9p
title: Rumex acetosella L.

description: Digital Specimen for the physical specimen hosted at Botanic Garden and Botanical Museum Berlin.
DOI: 10.3535/jjy-47q-5yn
title: Acer platanoides L.

description: Digital Specimen for the physical specimen hosted at Botanic Garden and Botanical Museum Berlin.
DOI: 10.17182/hepdata.96906.v1/t28
title: "Figure 14 ($\Lambda$)" of "Centrality dependence of charged hadron and strange hadron elliptic flow from sqrt(s_NN) = 200 GeV Au+Au collisions"

description: Fig14 $p_{T}$ dependence of $v_{2}$ of $\Lambda$ at 200 GeV.
description: We present STAR results on the elliptic flow $v_2$ of charged hadrons, strange and multi-strange particles from $\sqrt{s_{NN}} = 200$ GeV $Au+Au$ collisions at RHIC. The detailed study of the centrality dependence of $v_{2}$ over a broad transverse momentum range is presented. Comparison of different analysis methods are made in order to estimate systematic uncertainties. In order to discuss the non-flow effect, we have performed the first analysis of $v_{2}$ with the Lee-Yang Zero method for $K_{S}^{0}$ and $\Lambda$. In the relatively low $p_{T}$ region, $p_{T} \le 2$ GeV/c, a scaling with $m_{T}−m$ is observed for identified hadrons in each centrality bin studied. However, we do not observe $v_{2}(p_{T})$ scaled by the participant eccentricity to be independent of centrality. At higher $p_{T}$ , $2 \le p_{T} \le 6$ GeV/c, $v_{2}$ scales 3 with quark number for all hadrons studied. For the multi-strange hadron $\Omega$, which does not suffer appreciable hadronic interactions, the values of $v_{2}$ are consistent with both $m_{T}−m$ scaling at low $p_{T}$ and number-of-quark scaling at intermediate $p_{T}$. As a function of collision centrality, an increase of $p_{T}$-integrated $v_{2}$ scaled by the participant eccentricity has been observed, indicating a stronger collective flow in more central $Au+Au$ collisions.
DOI: 10.17182/hepdata.96955.v1/t1
title: "Figure 5 (200 GeV)" of "Harmonic decomposition of three-particle azimuthal correlations at RHIC"

description: The centrality dependence of the C$_{m,n,m+n}$ correlations versus N$_{part}$ for charged hadrons with p$_{T}&gt;0.2$ GeV/c and $\eta&lt;1$ from 200 GeV Au+Au collisions.
description: No data abstract available.
DOI: 10.17182/hepdata.96955.v1/t2
title: "Figure 5 (62.4 GeV)" of "Harmonic decomposition of three-particle azimuthal correlations at RHIC"

description: The centrality dependence of the C$_{m,n,m+n}$ correlations versus N$_{part}$ for charged hadrons with p$_{T}&gt;0.2$ GeV/c and $\eta&lt;1$ from 62.4 GeV Au+Au collisions.
description: No data abstract available.
DOI: 10.17182/hepdata.96955.v1/t3
title: "Figure 5 (39 GeV)" of "Harmonic decomposition of three-particle azimuthal correlations at RHIC"

description: The centrality dependence of the C$_{m,n,m+n}$ correlations versus N$_{part}$ for charged hadrons with p$_{T}&gt;0.2$ GeV/c and $\eta&lt;1$ from 39 GeV Au+Au collisions.
description: No data abstract available.
DOI: 10.17182/hepdata.96955.v1/t4
title: "Figure 5 (27 GeV)" of "Harmonic decomposition of three-particle azimuthal correlations at RHIC"

description: The centrality dependence of the C$_{m,n,m+n}$ correlations versus N$_{part}$ for charged hadrons with p$_{T}&gt;0.2$ GeV/c and $\eta&lt;1$ from 27 GeV Au+Au collisions.
description: No data abstract available.
DOI: 10.17182/hepdata.96955.v1/t5
title: "Figure 6 (19.6 GeV)" of "Harmonic decomposition of three-particle azimuthal correlations at RHIC"

description: The centrality dependence of the C$_{m,n,m+n}$ correlations versus N$_{part}$ for charged hadrons with p$_{T}&gt;0.2$ GeV/c and $\eta&lt;1$ from 19.6 GeV Au+Au collisions.
description: No data abstract available.
DOI: 10.17182/hepdata.96955.v1/t6
title: "Figure 6 (14.5 GeV)" of "Harmonic decomposition of three-particle azimuthal correlations at RHIC"

description: The centrality dependence of the C$_{m,n,m+n}$ correlations versus N$_{part}$ for charged hadrons with p$_{T}&gt;0.2$ GeV/c and $\eta&lt;1$ from 14.5 GeV Au+Au collisions.
description: No data abstract available.
DOI: 10.17182/hepdata.96955.v1/t7
title: "Figure 6 (11.5 GeV)" of "Harmonic decomposition of three-particle azimuthal correlations at RHIC"

description: The centrality dependence of the C$_{m,n,m+n}$ correlations versus N$_{part}$ for charged hadrons with p$_{T}&gt;0.2$ GeV/c and $\eta&lt;1$ from 11.5 GeV Au+Au collisions.
description: No data abstract available.
DOI: 10.17182/hepdata.96955.v1/t8
title: "Figure 6 (7.7 GeV)" of "Harmonic decomposition of three-particle azimuthal correlations at RHIC"

description: The centrality dependence of the C$_{m,n,m+n}$ correlations versus N$_{part}$ for charged hadrons with p$_{T}&gt;0.2$ GeV/c and $\eta&lt;1$ from 7.7 GeV Au+Au collisions.
description: No data abstract available.
DOI: 10.3535/1jh-h6q-qv1
title: Medicago minima (L.) Bartal.

description: Digital Specimen for the physical specimen hosted at Botanic Garden and Botanical Museum Berlin.
DOI: 10.17182/hepdata.96955.v1/t10
title: "Figure 8 (left)" of "Harmonic decomposition of three-particle azimuthal correlations at RHIC"

description: Three-particle azimuthal correlations C$_{1,2,3}$ as a function of the particle one p$_{T}$ for charged hadrons with p$_{T}&gt;0.2$ GeV/c and $\eta&lt;1$.
description: No data abstract available.
DOI: 10.17182/hepdata.96955.v1/t11
title: "Figure 8 (right)" of "Harmonic decomposition of three-particle azimuthal correlations at RHIC"

description: Three-particle azimuthal correlations C$_{1,2,3}$ as a function of the particle two p$_{T}$ for charged hadrons with p$_{T}&gt;0.2$ GeV/c and $\eta&lt;1$.
description: No data abstract available.
DOI: 10.17182/hepdata.96955.v1/t12
title: "Figure 9" of "Harmonic decomposition of three-particle azimuthal correlations at RHIC"

description: Three-particle azimuthal correlations C$_{2,2,4}$ as a function of the first particles p$_{T}$ for charged hadrons with p$_{T}&gt;0.2$ GeV/c and $\eta&lt;1$.
description: No data abstract available.
DOI: 10.17182/hepdata.96955.v1/t13
title: "Figure 10 (left)" of "Harmonic decomposition of three-particle azimuthal correlations at RHIC"

description: Three-particle azimuthal correlations C$_{2,3,5}$ as a function of the particle one p$_{T}$ for charged hadrons with p$_{T}&gt;0.2$ GeV/c and $\eta&lt;1$.
description: No data abstract available.
DOI: 10.17182/hepdata.96955.v1/t14
title: "Figure 10 (right)" of "Harmonic decomposition of three-particle azimuthal correlations at RHIC"

description: Three-particle azimuthal correlations C$_{2,3,5}$ as a function of the particle two p$_{T}$ for charged hadrons with p$_{T}&gt;0.2$ GeV/c and $\eta&lt;1$.
description: No data abstract available.
DOI: 10.17182/hepdata.96955.v1/t9
title: "Figure 7" of "Harmonic decomposition of three-particle azimuthal correlations at RHIC"

description: Three-particle azimuthal correlations C$_{1,1,2}$ as a function of the first particles p$_{T}$ for charged hadrons with p$_{T}&gt;0.2$ GeV/c and $\eta&lt;1$.
description: No data abstract available.
DOI: 10.3535/3tr-vb6-gae
title: Prunus serotina Ehrh.

description: Digital Specimen for the physical specimen hosted at Botanic Garden and Botanical Museum Berlin.
DOI: 10.3535/yy2-tmt-ljs
title: Quercus robur L.

description: Digital Specimen for the physical specimen hosted at Botanic Garden and Botanical Museum Berlin.
DOI: 10.17182/hepdata.96955.v1/t15
title: "Figure 14 (left)" of "Harmonic decomposition of three-particle azimuthal correlations at RHIC"

description: The $\sqrt{s_{NN}}$ and centrality dependence of $v_{1}\{2\}^2$ after short-range correlations,predominantly from quantum and Coulomb effects, have been subtracted.
description: No data abstract available.
DOI: 10.17182/hepdata.96955.v1/t16
title: "Figure 14 (right)" of "Harmonic decomposition of three-particle azimuthal correlations at RHIC"

description: The $\sqrt{s_{NN}}$ and centrality dependence of $v_{2}\{2\}^2$ after short-range correlations,predominantly from quantum and Coulomb effects, have been subtracted.
description: No data abstract available.
DOI: 10.17182/hepdata.96955.v1/t17
title: "Figure 15 (left)" of "Harmonic decomposition of three-particle azimuthal correlations at RHIC"

description: The $\sqrt{s_{NN}}$ and centrality dependence of $v_{4}\{2\}^2$ after short-range correlations,predominantly from quantum and Coulomb effects, have been subtracted.
description: No data abstract available.
DOI: 10.17182/hepdata.96955.v1/t18
title: "Figure 15 (right)" of "Harmonic decomposition of three-particle azimuthal correlations at RHIC"

description: The $\sqrt{s_{NN}}$ and centrality dependence of $v_{5}\{2\}^2$ after short-range correlations,predominantly from quantum and Coulomb effects, have been subtracted.
description: No data abstract available.