cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.98575.v1/t19
title: "Figure 9.0.0" of "Charged and strange hadron elliptic flow in Cu+Cu collisions at $\sqrt{s_{NN}}$ = 62.4 and 200 GeV"

description: K0S azimuthal anisotropy v2 vs pT in 0-60% central Cu+Cu collisions at 200 GeV.
description: We present the results of an elliptic flow, v2, analysis of Cu+Cu collisions recorded with the solenoidal tracker detector (STAR) at the BNL Relativistic Heavy Ion Collider at $\sqrt{s_{NN}}$ = 62.4 and 200 GeV. Elliptic flow as a function of transverse momentum, v2(pT), is reported for different collision centralities for charged hadrons h± and strangeness-ontaining hadrons K_0^S, Lambda, Xi, and phi in the midrapidity region |eta| &lt; 1.0. Significant reduction in systematic uncertainty of the measurement due to nonflow effects has been achieved by correlating particles at midrapidity, |eta| &lt; 1.0, with those at forward rapidity, 2.5 &lt; |eta| &lt; 4.0. We also present azimuthal correlations in p+p collisions at $\sqrt{s}$ = 200 GeV to help in estimating nonflow effects. To study the system-size dependence of elliptic flow, we present a detailed comparison with previously published results from Au+Au collisions at $\sqrt{s_{NN}}$ = 200GeV. We observe that v2(pT) of strange hadrons has similar scaling properties as were first observed in Au+Au collisions, that is, (i) at low transverse momenta, pT &lt; 2 GeV/c, v2 scales with transverse kinetic energy, mT−m, and (ii) atintermediate pT, 2 &lt; pT &lt; 4 GeV/c, it scales with the number of constituent quarks, nq. We have found that ideal hydrodynamic calculations fail to reproduce the centrality dependence of v2 (pT) for K_0^S and Lambda. Eccentricity scaled v2 values, v2/epsilon, are larger in more central collisions, suggesting stronger collective flow develops in more central collisions. The comparison with Au+Au collisions, which go further in density, shows that v2/epsilon depends on the system size, that is, the number of participants Npart. This indicates that the ideal hydrodynamic limit is not reached in Cu+Cu collisions, presumably because the assumption of thermalization is not attained.
DOI: 10.17182/hepdata.98575.v1/t20
title: "Figure 9.0.1" of "Charged and strange hadron elliptic flow in Cu+Cu collisions at $\sqrt{s_{NN}}$ = 62.4 and 200 GeV"

description: K0S azimuthal anisotropy v2 vs pT in 0-20% central Cu+Cu collisions at 200 GeV.
description: We present the results of an elliptic flow, v2, analysis of Cu+Cu collisions recorded with the solenoidal tracker detector (STAR) at the BNL Relativistic Heavy Ion Collider at $\sqrt{s_{NN}}$ = 62.4 and 200 GeV. Elliptic flow as a function of transverse momentum, v2(pT), is reported for different collision centralities for charged hadrons h± and strangeness-ontaining hadrons K_0^S, Lambda, Xi, and phi in the midrapidity region |eta| &lt; 1.0. Significant reduction in systematic uncertainty of the measurement due to nonflow effects has been achieved by correlating particles at midrapidity, |eta| &lt; 1.0, with those at forward rapidity, 2.5 &lt; |eta| &lt; 4.0. We also present azimuthal correlations in p+p collisions at $\sqrt{s}$ = 200 GeV to help in estimating nonflow effects. To study the system-size dependence of elliptic flow, we present a detailed comparison with previously published results from Au+Au collisions at $\sqrt{s_{NN}}$ = 200GeV. We observe that v2(pT) of strange hadrons has similar scaling properties as were first observed in Au+Au collisions, that is, (i) at low transverse momenta, pT &lt; 2 GeV/c, v2 scales with transverse kinetic energy, mT−m, and (ii) atintermediate pT, 2 &lt; pT &lt; 4 GeV/c, it scales with the number of constituent quarks, nq. We have found that ideal hydrodynamic calculations fail to reproduce the centrality dependence of v2 (pT) for K_0^S and Lambda. Eccentricity scaled v2 values, v2/epsilon, are larger in more central collisions, suggesting stronger collective flow develops in more central collisions. The comparison with Au+Au collisions, which go further in density, shows that v2/epsilon depends on the system size, that is, the number of participants Npart. This indicates that the ideal hydrodynamic limit is not reached in Cu+Cu collisions, presumably because the assumption of thermalization is not attained.
DOI: 10.17182/hepdata.98575.v1/t21
title: "Figure 9.0.2" of "Charged and strange hadron elliptic flow in Cu+Cu collisions at $\sqrt{s_{NN}}$ = 62.4 and 200 GeV"

description: K0S azimuthal anisotropy v2 vs pT in 20-60% central Cu+Cu collisions at 200 GeV.
description: We present the results of an elliptic flow, v2, analysis of Cu+Cu collisions recorded with the solenoidal tracker detector (STAR) at the BNL Relativistic Heavy Ion Collider at $\sqrt{s_{NN}}$ = 62.4 and 200 GeV. Elliptic flow as a function of transverse momentum, v2(pT), is reported for different collision centralities for charged hadrons h± and strangeness-ontaining hadrons K_0^S, Lambda, Xi, and phi in the midrapidity region |eta| &lt; 1.0. Significant reduction in systematic uncertainty of the measurement due to nonflow effects has been achieved by correlating particles at midrapidity, |eta| &lt; 1.0, with those at forward rapidity, 2.5 &lt; |eta| &lt; 4.0. We also present azimuthal correlations in p+p collisions at $\sqrt{s}$ = 200 GeV to help in estimating nonflow effects. To study the system-size dependence of elliptic flow, we present a detailed comparison with previously published results from Au+Au collisions at $\sqrt{s_{NN}}$ = 200GeV. We observe that v2(pT) of strange hadrons has similar scaling properties as were first observed in Au+Au collisions, that is, (i) at low transverse momenta, pT &lt; 2 GeV/c, v2 scales with transverse kinetic energy, mT−m, and (ii) atintermediate pT, 2 &lt; pT &lt; 4 GeV/c, it scales with the number of constituent quarks, nq. We have found that ideal hydrodynamic calculations fail to reproduce the centrality dependence of v2 (pT) for K_0^S and Lambda. Eccentricity scaled v2 values, v2/epsilon, are larger in more central collisions, suggesting stronger collective flow develops in more central collisions. The comparison with Au+Au collisions, which go further in density, shows that v2/epsilon depends on the system size, that is, the number of participants Npart. This indicates that the ideal hydrodynamic limit is not reached in Cu+Cu collisions, presumably because the assumption of thermalization is not attained.
DOI: 10.3535/vny-8ml-5xb
title: Pyrus salicifolia Pall.

description: Digital Specimen for the physical specimen hosted at Botanic Garden and Botanical Museum Berlin.
DOI: 10.3535/xbd-l5c-qpn
title: Pyrus salicifolia Pall.

description: Digital Specimen for the physical specimen hosted at Botanic Garden and Botanical Museum Berlin.
DOI: 10.17182/hepdata.98575.v1/t22
title: "Figure 9.1.0" of "Charged and strange hadron elliptic flow in Cu+Cu collisions at $\sqrt{s_{NN}}$ = 62.4 and 200 GeV"

description: Lambda azimuthal anisotropy v2 vs pT in 0-60% central Cu+Cu collisions at 200 GeV.
description: We present the results of an elliptic flow, v2, analysis of Cu+Cu collisions recorded with the solenoidal tracker detector (STAR) at the BNL Relativistic Heavy Ion Collider at $\sqrt{s_{NN}}$ = 62.4 and 200 GeV. Elliptic flow as a function of transverse momentum, v2(pT), is reported for different collision centralities for charged hadrons h± and strangeness-ontaining hadrons K_0^S, Lambda, Xi, and phi in the midrapidity region |eta| &lt; 1.0. Significant reduction in systematic uncertainty of the measurement due to nonflow effects has been achieved by correlating particles at midrapidity, |eta| &lt; 1.0, with those at forward rapidity, 2.5 &lt; |eta| &lt; 4.0. We also present azimuthal correlations in p+p collisions at $\sqrt{s}$ = 200 GeV to help in estimating nonflow effects. To study the system-size dependence of elliptic flow, we present a detailed comparison with previously published results from Au+Au collisions at $\sqrt{s_{NN}}$ = 200GeV. We observe that v2(pT) of strange hadrons has similar scaling properties as were first observed in Au+Au collisions, that is, (i) at low transverse momenta, pT &lt; 2 GeV/c, v2 scales with transverse kinetic energy, mT−m, and (ii) atintermediate pT, 2 &lt; pT &lt; 4 GeV/c, it scales with the number of constituent quarks, nq. We have found that ideal hydrodynamic calculations fail to reproduce the centrality dependence of v2 (pT) for K_0^S and Lambda. Eccentricity scaled v2 values, v2/epsilon, are larger in more central collisions, suggesting stronger collective flow develops in more central collisions. The comparison with Au+Au collisions, which go further in density, shows that v2/epsilon depends on the system size, that is, the number of participants Npart. This indicates that the ideal hydrodynamic limit is not reached in Cu+Cu collisions, presumably because the assumption of thermalization is not attained.
DOI: 10.17182/hepdata.98575.v1/t23
title: "Figure 9.1.1" of "Charged and strange hadron elliptic flow in Cu+Cu collisions at $\sqrt{s_{NN}}$ = 62.4 and 200 GeV"

description: Lambda azimuthal anisotropy v2 vs pT in 0-20% central Cu+Cu collisions at 200 GeV.
description: We present the results of an elliptic flow, v2, analysis of Cu+Cu collisions recorded with the solenoidal tracker detector (STAR) at the BNL Relativistic Heavy Ion Collider at $\sqrt{s_{NN}}$ = 62.4 and 200 GeV. Elliptic flow as a function of transverse momentum, v2(pT), is reported for different collision centralities for charged hadrons h± and strangeness-ontaining hadrons K_0^S, Lambda, Xi, and phi in the midrapidity region |eta| &lt; 1.0. Significant reduction in systematic uncertainty of the measurement due to nonflow effects has been achieved by correlating particles at midrapidity, |eta| &lt; 1.0, with those at forward rapidity, 2.5 &lt; |eta| &lt; 4.0. We also present azimuthal correlations in p+p collisions at $\sqrt{s}$ = 200 GeV to help in estimating nonflow effects. To study the system-size dependence of elliptic flow, we present a detailed comparison with previously published results from Au+Au collisions at $\sqrt{s_{NN}}$ = 200GeV. We observe that v2(pT) of strange hadrons has similar scaling properties as were first observed in Au+Au collisions, that is, (i) at low transverse momenta, pT &lt; 2 GeV/c, v2 scales with transverse kinetic energy, mT−m, and (ii) atintermediate pT, 2 &lt; pT &lt; 4 GeV/c, it scales with the number of constituent quarks, nq. We have found that ideal hydrodynamic calculations fail to reproduce the centrality dependence of v2 (pT) for K_0^S and Lambda. Eccentricity scaled v2 values, v2/epsilon, are larger in more central collisions, suggesting stronger collective flow develops in more central collisions. The comparison with Au+Au collisions, which go further in density, shows that v2/epsilon depends on the system size, that is, the number of participants Npart. This indicates that the ideal hydrodynamic limit is not reached in Cu+Cu collisions, presumably because the assumption of thermalization is not attained.
DOI: 10.17182/hepdata.98575.v1/t24
title: "Figure 9.1.2" of "Charged and strange hadron elliptic flow in Cu+Cu collisions at $\sqrt{s_{NN}}$ = 62.4 and 200 GeV"

description: Lambda azimuthal anisotropy v2 vs pT in 20-60% central Cu+Cu collisions at 200 GeV.
description: We present the results of an elliptic flow, v2, analysis of Cu+Cu collisions recorded with the solenoidal tracker detector (STAR) at the BNL Relativistic Heavy Ion Collider at $\sqrt{s_{NN}}$ = 62.4 and 200 GeV. Elliptic flow as a function of transverse momentum, v2(pT), is reported for different collision centralities for charged hadrons h± and strangeness-ontaining hadrons K_0^S, Lambda, Xi, and phi in the midrapidity region |eta| &lt; 1.0. Significant reduction in systematic uncertainty of the measurement due to nonflow effects has been achieved by correlating particles at midrapidity, |eta| &lt; 1.0, with those at forward rapidity, 2.5 &lt; |eta| &lt; 4.0. We also present azimuthal correlations in p+p collisions at $\sqrt{s}$ = 200 GeV to help in estimating nonflow effects. To study the system-size dependence of elliptic flow, we present a detailed comparison with previously published results from Au+Au collisions at $\sqrt{s_{NN}}$ = 200GeV. We observe that v2(pT) of strange hadrons has similar scaling properties as were first observed in Au+Au collisions, that is, (i) at low transverse momenta, pT &lt; 2 GeV/c, v2 scales with transverse kinetic energy, mT−m, and (ii) atintermediate pT, 2 &lt; pT &lt; 4 GeV/c, it scales with the number of constituent quarks, nq. We have found that ideal hydrodynamic calculations fail to reproduce the centrality dependence of v2 (pT) for K_0^S and Lambda. Eccentricity scaled v2 values, v2/epsilon, are larger in more central collisions, suggesting stronger collective flow develops in more central collisions. The comparison with Au+Au collisions, which go further in density, shows that v2/epsilon depends on the system size, that is, the number of participants Npart. This indicates that the ideal hydrodynamic limit is not reached in Cu+Cu collisions, presumably because the assumption of thermalization is not attained.
DOI: 10.17182/hepdata.98575.v1/t25
title: "Figure 9.2" of "Charged and strange hadron elliptic flow in Cu+Cu collisions at $\sqrt{s_{NN}}$ = 62.4 and 200 GeV"

description: Xi azimuthal anisotropy v2 vs pT in 0-60% central Cu+Cu collisions at 200 GeV.
description: We present the results of an elliptic flow, v2, analysis of Cu+Cu collisions recorded with the solenoidal tracker detector (STAR) at the BNL Relativistic Heavy Ion Collider at $\sqrt{s_{NN}}$ = 62.4 and 200 GeV. Elliptic flow as a function of transverse momentum, v2(pT), is reported for different collision centralities for charged hadrons h± and strangeness-ontaining hadrons K_0^S, Lambda, Xi, and phi in the midrapidity region |eta| &lt; 1.0. Significant reduction in systematic uncertainty of the measurement due to nonflow effects has been achieved by correlating particles at midrapidity, |eta| &lt; 1.0, with those at forward rapidity, 2.5 &lt; |eta| &lt; 4.0. We also present azimuthal correlations in p+p collisions at $\sqrt{s}$ = 200 GeV to help in estimating nonflow effects. To study the system-size dependence of elliptic flow, we present a detailed comparison with previously published results from Au+Au collisions at $\sqrt{s_{NN}}$ = 200GeV. We observe that v2(pT) of strange hadrons has similar scaling properties as were first observed in Au+Au collisions, that is, (i) at low transverse momenta, pT &lt; 2 GeV/c, v2 scales with transverse kinetic energy, mT−m, and (ii) atintermediate pT, 2 &lt; pT &lt; 4 GeV/c, it scales with the number of constituent quarks, nq. We have found that ideal hydrodynamic calculations fail to reproduce the centrality dependence of v2 (pT) for K_0^S and Lambda. Eccentricity scaled v2 values, v2/epsilon, are larger in more central collisions, suggesting stronger collective flow develops in more central collisions. The comparison with Au+Au collisions, which go further in density, shows that v2/epsilon depends on the system size, that is, the number of participants Npart. This indicates that the ideal hydrodynamic limit is not reached in Cu+Cu collisions, presumably because the assumption of thermalization is not attained.
DOI: 10.17182/hepdata.98575.v1/t26
title: "Figure 9.3" of "Charged and strange hadron elliptic flow in Cu+Cu collisions at $\sqrt{s_{NN}}$ = 62.4 and 200 GeV"

description: phi azimuthal anisotropy v2 vs pT in 0-60% central Cu+Cu collisions at 200 GeV.
description: We present the results of an elliptic flow, v2, analysis of Cu+Cu collisions recorded with the solenoidal tracker detector (STAR) at the BNL Relativistic Heavy Ion Collider at $\sqrt{s_{NN}}$ = 62.4 and 200 GeV. Elliptic flow as a function of transverse momentum, v2(pT), is reported for different collision centralities for charged hadrons h± and strangeness-ontaining hadrons K_0^S, Lambda, Xi, and phi in the midrapidity region |eta| &lt; 1.0. Significant reduction in systematic uncertainty of the measurement due to nonflow effects has been achieved by correlating particles at midrapidity, |eta| &lt; 1.0, with those at forward rapidity, 2.5 &lt; |eta| &lt; 4.0. We also present azimuthal correlations in p+p collisions at $\sqrt{s}$ = 200 GeV to help in estimating nonflow effects. To study the system-size dependence of elliptic flow, we present a detailed comparison with previously published results from Au+Au collisions at $\sqrt{s_{NN}}$ = 200GeV. We observe that v2(pT) of strange hadrons has similar scaling properties as were first observed in Au+Au collisions, that is, (i) at low transverse momenta, pT &lt; 2 GeV/c, v2 scales with transverse kinetic energy, mT−m, and (ii) atintermediate pT, 2 &lt; pT &lt; 4 GeV/c, it scales with the number of constituent quarks, nq. We have found that ideal hydrodynamic calculations fail to reproduce the centrality dependence of v2 (pT) for K_0^S and Lambda. Eccentricity scaled v2 values, v2/epsilon, are larger in more central collisions, suggesting stronger collective flow develops in more central collisions. The comparison with Au+Au collisions, which go further in density, shows that v2/epsilon depends on the system size, that is, the number of participants Npart. This indicates that the ideal hydrodynamic limit is not reached in Cu+Cu collisions, presumably because the assumption of thermalization is not attained.
DOI: 10.17182/hepdata.98576.v1/t1
title: "Figure 1" of "Evidence from d + Au measurements for final-state suppression of high p(T) hadrons in Au + Au collisions at RHIC."

description: Uncorrected charged particle multiplicity distributions measured in −3.8 &lt; $\eta$ &lt; −2.8 (Au-direction) for d+Au collisions. Points are for minimum bias (triangles) and peripheral (circles, ZDC-d single neutron) collisions. Both are normalized to the total number of d+Au collisions. Histograms are Glauber model calculations.
description: We report measurements of single-particle inclusive spectra and two-particle azimuthal distributions of charged hadrons at high transverse momentum (high $p_{T}$ ) in minimum bias and central d+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. The inclusive yield is enhanced in d+Au collisions relative to binary-scaled p+p collisions, while the two-particle azimuthal distributions are very similar to those observed in p+p collisions. These results demonstrate that the strong suppression of the inclusive yield and back-to-back correlations at high $p_{T}$ previously observed in central Au+Au collisions are due to final-state interactions with the dense medium generated in such collisions.
DOI: 10.25549/vercoutere-ouc1sto1770227
title: Therapeutic Artworks

description: This collection includes over 900 pieces of art that were created by patients at the Atascadero State Hospital (ASH) in the mid-1950’s.  The artists were under the treatment of Albert R. Vercoutere who used the technique of providing photos from magazines for the patients to use as inspiration for their own artwork. Although not trained in the use of art therapy and during a time when art therapy was a new approach, Vercoutere often utilized art as a mechanism for working with his patients. The artwork was created during a time when psychotropic drugs were not yet available as treatment options for mental health patients.
DOI: 10.3535/qsn-zty-mk3
title: Pyrus communis subsp. caucasica (Fed.) Browicz

description: Digital Specimen for the physical specimen hosted at Botanic Garden and Botanical Museum Berlin.
DOI: 10.3535/vy3-l8x-scc
title: Pyrus oxyprion Woronow

description: Digital Specimen for the physical specimen hosted at Botanic Garden and Botanical Museum Berlin.
DOI: 10.17182/hepdata.98576.v1/t2
title: "Figure 2" of "Evidence from d + Au measurements for final-state suppression of high p(T) hadrons in Au + Au collisions at RHIC."

description: Inclusive $p_{T}$ distributions for minimum bias and central d+Au collisions, and non-singly diffractive p+p collisions. Hash marks at the top indicate bin boundaries for $p_{T}$ &gt; 3.8 GeV/c.
description: We report measurements of single-particle inclusive spectra and two-particle azimuthal distributions of charged hadrons at high transverse momentum (high $p_{T}$ ) in minimum bias and central d+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. The inclusive yield is enhanced in d+Au collisions relative to binary-scaled p+p collisions, while the two-particle azimuthal distributions are very similar to those observed in p+p collisions. These results demonstrate that the strong suppression of the inclusive yield and back-to-back correlations at high $p_{T}$ previously observed in central Au+Au collisions are due to final-state interactions with the dense medium generated in such collisions.
DOI: 10.17182/hepdata.98576.v1/t3
title: "Figure 3" of "Evidence from d + Au measurements for final-state suppression of high p(T) hadrons in Au + Au collisions at RHIC."

description: $R_{AB}(p_{T})$ from Eq. 1 for minimum bias and central d+Au collisions, and central Au+Au collisions. The minimum bias d+Au data are displaced 100 MeV/c to the right for clarity. The error bars are the quadrature sum of the statistical and point-to-point systematic uncertainties. The bands show the normalization uncertainties, which are highly correlated point-to-point and between the two d+Au distributions.
description: We report measurements of single-particle inclusive spectra and two-particle azimuthal distributions of charged hadrons at high transverse momentum (high $p_{T}$ ) in minimum bias and central d+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. The inclusive yield is enhanced in d+Au collisions relative to binary-scaled p+p collisions, while the two-particle azimuthal distributions are very similar to those observed in p+p collisions. These results demonstrate that the strong suppression of the inclusive yield and back-to-back correlations at high $p_{T}$ previously observed in central Au+Au collisions are due to final-state interactions with the dense medium generated in such collisions.
DOI: 10.17182/hepdata.98576.v1/t4
title: "Figure 4a" of "Evidence from d + Au measurements for final-state suppression of high p(T) hadrons in Au + Au collisions at RHIC."

description: Efficiency corrected two-particle azimuthal distributions for minimum bias and central d+Au collisions, and for p+p collisions. Curves are fits using Eq. 3, with parameters given in Table I. Trigger particles are selected with 4 GeV/c &lt; $p_{T}$ (trig) &lt; 6 GeV/c, while associated particles are selected within 2 GeV/c &lt; $p_{T}$ &lt; $p_{T}$ (trig), with |$\eta$| &lt; 0.7 for both sets. Only statistical errors are listed. Normalization uncertainties are less than 5%.
description: We report measurements of single-particle inclusive spectra and two-particle azimuthal distributions of charged hadrons at high transverse momentum (high $p_{T}$ ) in minimum bias and central d+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. The inclusive yield is enhanced in d+Au collisions relative to binary-scaled p+p collisions, while the two-particle azimuthal distributions are very similar to those observed in p+p collisions. These results demonstrate that the strong suppression of the inclusive yield and back-to-back correlations at high $p_{T}$ previously observed in central Au+Au collisions are due to final-state interactions with the dense medium generated in such collisions.