cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.3535/7rz-fl7-dxm
title: Pyrus sachokiana Kuth.

description: Digital Specimen for the physical specimen hosted at Botanic Garden and Botanical Museum Berlin.
DOI: 10.3535/xte-2z0-4q8
title: Pyrus demetrii Kuth.

description: Digital Specimen for the physical specimen hosted at Botanic Garden and Botanical Museum Berlin.
DOI: 10.25549/vercoutere-ouc1sto1770229
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/ppb-724-nnb
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/tjh-b4h-b5d
title: Pyrus ketzkhovelii S. Kuthath.

description: Digital Specimen for the physical specimen hosted at Botanic Garden and Botanical Museum Berlin.
DOI: 10.3535/mxg-70y-8fb
title: Pyrus sachokiana Kuth.

description: Digital Specimen for the physical specimen hosted at Botanic Garden and Botanical Museum Berlin.
DOI: 10.25549/vercoutere-ouc1sto1770107
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/e4m-dqs-731
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/ecd-hez-935
title: Pyrus salicifolia Pall.

description: Digital Specimen for the physical specimen hosted at Botanic Garden and Botanical Museum Berlin.
DOI: 10.3535/0p4-xjl-y6e
title: Pyrus communis subsp. caucasica (Fed.) Browicz

description: Digital Specimen for the physical specimen hosted at Botanic Garden and Botanical Museum Berlin.
DOI: 10.17182/hepdata.98574.v1/t1
title: "Figure 2" of "Measurement of J/{psi} Azimuthal Anisotropy in Au+Au Collisions at {sqrt{s_{NN}}} = 200 GeV"

description: J/Psi azimuthal anisotropy v2 vs pT measured via the dielectron channel in 0-10%, 10-40%, and 40-80% central Au+Au collisions at 200 GeV. The brackets represent systematic errors. The boxes show the estimated maximum possible range of v2 if the nonflow influence is corrected. The mean pT in each bin for v2 calculation is drawn, but is shifted a little for some centralities so that all points can be seen clearly.
description: The measurement of J/Psi azimuthal anisotropy is presented as a function of transverse momentum for different centralities in Au+Au collisions at \sqrt{s_{NN}}=200 GeV. The measured J/Psi elliptic flow is consistent with zero within errors for transverse momentum between 2 and 10 GeV/c. Our measurement suggests that J/Psi particles with relatively large transverse momenta are not dominantly produced by coalescence from thermalized charm quarks, when comparing to model calculations.
DOI: 10.3535/6wm-k4p-f5j
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/fhg-411-h8p
title: Pyrus communis subsp. caucasica (Fed.) Browicz

description: Digital Specimen for the physical specimen hosted at Botanic Garden and Botanical Museum Berlin.
DOI: 10.17182/hepdata.98574.v1/t2
title: "Figure 3" of "Measurement of J/{psi} Azimuthal Anisotropy in Au+Au Collisions at {sqrt{s_{NN}}} = 200 GeV"

description: J/Psi azimuthal anisotropy v2 vs pT measured via the dielectron channel in 0-80% central Au+Au collisions at 200 GeV. The brackets represent systematic errors. The boxes show the estimated maximum possible range of v2 if the nonflow influence is corrected.
description: The measurement of J/Psi azimuthal anisotropy is presented as a function of transverse momentum for different centralities in Au+Au collisions at \sqrt{s_{NN}}=200 GeV. The measured J/Psi elliptic flow is consistent with zero within errors for transverse momentum between 2 and 10 GeV/c. Our measurement suggests that J/Psi particles with relatively large transverse momenta are not dominantly produced by coalescence from thermalized charm quarks, when comparing to model calculations.
DOI: 10.17182/hepdata.98575.v1/t1
title: "Figure 2" of "Charged and strange hadron elliptic flow in Cu+Cu collisions at $\sqrt{s_{NN}}$ = 62.4 and 200 GeV"

description: Charged hadron azimuthal correlations as a function of pT in 0-60% Cu+Cu and p+p collisions at 200 GeV using TPC and FTPC flow vectors.
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/t2
title: "Figure 3.0" of "Charged and strange hadron elliptic flow in Cu+Cu collisions at $\sqrt{s_{NN}}$ = 62.4 and 200 GeV"

description: Charged hadron azimuthal anisotropy v2 as a function of pT in 0-60% Cu+Cu collisions at 200 GeV using TPC flow vectors, and those with subtracting the azimuthal correlations in p+p collisions.
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/t3
title: "Figure 3.1" of "Charged and strange hadron elliptic flow in Cu+Cu collisions at $\sqrt{s_{NN}}$ = 62.4 and 200 GeV"

description: Charged hadron azimuthal anisotropy v2 as a function of pT in 0-60% Cu+Cu collisions at 200 GeV using FTPC flow vectors, and those with subtracting the azimuthal correlations in p+p collisions.
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/t4
title: "Figure 4.0" of "Charged and strange hadron elliptic flow in Cu+Cu collisions at $\sqrt{s_{NN}}$ = 62.4 and 200 GeV"

description: Charged hadron azimuthal anisotropy v2 as a function of pT in 50-60% Cu+Cu collisions at 200 GeV using FTPC flow vectors, and that with subtracting the azimuthal correlations in p+p collisions.
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/t5
title: "Figure 4.1" of "Charged and strange hadron elliptic flow in Cu+Cu collisions at $\sqrt{s_{NN}}$ = 62.4 and 200 GeV"

description: Charged hadron azimuthal anisotropy v2 as a function of pT in 40-50% Cu+Cu collisions at 200 GeV using FTPC flow vectors, and that with subtracting the azimuthal correlations in p+p collisions.
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/t6
title: "Figure 4.2" of "Charged and strange hadron elliptic flow in Cu+Cu collisions at $\sqrt{s_{NN}}$ = 62.4 and 200 GeV"

description: Charged hadron azimuthal anisotropy v2 as a function of pT in 30-40% Cu+Cu collisions at 200 GeV using FTPC flow vectors, and that with subtracting the azimuthal correlations in p+p collisions.
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: 10.25549/vercoutere-ouc1sto1769495
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/cg8-pyc-lqf
title: Pyrus salicifolia Pall.

description: Digital Specimen for the physical specimen hosted at Botanic Garden and Botanical Museum Berlin.
DOI: 10.3535/f6b-ebv-wxh
title: Pyrus communis subsp. caucasica (Fed.) Browicz

description: Digital Specimen for the physical specimen hosted at Botanic Garden and Botanical Museum Berlin.
DOI: 10.17182/hepdata.98575.v1/t10
title: "Figure 6.0" of "Charged and strange hadron elliptic flow in Cu+Cu collisions at $\sqrt{s_{NN}}$ = 62.4 and 200 GeV"

description: Charged hadron azimuthal anisotropy v2 integrated over pT and eta vs centrality in Cu+Cu collisions at 200 GeV for the various methods.
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/t11
title: "Figure 6.1" of "Charged and strange hadron elliptic flow in Cu+Cu collisions at $\sqrt{s_{NN}}$ = 62.4 and 200 GeV"

description: Charged hadron azimuthal anisotropy v2 integrated over pT and eta vs centrality in Cu+Cu collisions at 62.4 GeV for the various methods.
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.