cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.96601.v1/t12
title: "Table 18" of "Transverse energy production and charged-particle multiplicity at midrapidity in various systems from $\sqrt{s_{NN}}=7.7$ to 200 GeV"

description: Multiplicity in Au+Au collisions at $\sqrt{s_{NN}}$ = 19.6 GeV
description: BNL-RHIC. Measurements of midrapidity charged particle multiplicity distributions, $dN_{ch}/d\eta$, and midrapidity transverse-energy distributions, $dE_T/d\eta$, are presented for a variety of collision systems and energies. Included are distributions for Au+Au collisions at $\sqrt{s_{NN}}$ = 200, 130, 62.4, 39, 27,19.6, 14.5, and 7.7 GeV, Cu+Cu collisions at $\sqrt{s_{NN}}$ = 200 and 62.4 GeV, Cu+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV, U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV, d+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV, $^3$He+Au collisions at $\sqrt{s_{NN}}$ 200 GeV, and p+p collisions at $\sqrt{s_{NN}}$ = 200 GeV. Centrality dependent distributions at midrapidity are presented in terms of the number of nucleon participants, Npart, and the number of constituent quark participants, $N_{qp}$. For all A+A collisions down to $\sqrt{s_{NN}}$ = 7.7 GeV, it is observed that the midrapidity data are better described by scaling with $N_{qp}$ than scaling with $N_{part}$. Also presented are estimates of the Bjorken energy density, $\epsilon_{BJ}$, and the ratio of $dET/d\eta$ to $dNch/d\eta$, the latter of which is seen to be constant as a function of centrality for all systems.
DOI: 10.17182/hepdata.96601.v1/t13
title: "Table 19" of "Transverse energy production and charged-particle multiplicity at midrapidity in various systems from $\sqrt{s_{NN}}=7.7$ to 200 GeV"

description: Transverse energy in Au+Au collisions at $\sqrt{s_{NN}}$ = 14.5 GeV
description: BNL-RHIC. Measurements of midrapidity charged particle multiplicity distributions, $dN_{ch}/d\eta$, and midrapidity transverse-energy distributions, $dE_T/d\eta$, are presented for a variety of collision systems and energies. Included are distributions for Au+Au collisions at $\sqrt{s_{NN}}$ = 200, 130, 62.4, 39, 27,19.6, 14.5, and 7.7 GeV, Cu+Cu collisions at $\sqrt{s_{NN}}$ = 200 and 62.4 GeV, Cu+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV, U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV, d+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV, $^3$He+Au collisions at $\sqrt{s_{NN}}$ 200 GeV, and p+p collisions at $\sqrt{s_{NN}}$ = 200 GeV. Centrality dependent distributions at midrapidity are presented in terms of the number of nucleon participants, Npart, and the number of constituent quark participants, $N_{qp}$. For all A+A collisions down to $\sqrt{s_{NN}}$ = 7.7 GeV, it is observed that the midrapidity data are better described by scaling with $N_{qp}$ than scaling with $N_{part}$. Also presented are estimates of the Bjorken energy density, $\epsilon_{BJ}$, and the ratio of $dET/d\eta$ to $dNch/d\eta$, the latter of which is seen to be constant as a function of centrality for all systems.
DOI: 10.17182/hepdata.96601.v1/t7
title: "Table 13" of "Transverse energy production and charged-particle multiplicity at midrapidity in various systems from $\sqrt{s_{NN}}=7.7$ to 200 GeV"

description: Transverse energy in Au+Au collisions at $\sqrt{s_{NN}}$ = 39 GeV
description: BNL-RHIC. Measurements of midrapidity charged particle multiplicity distributions, $dN_{ch}/d\eta$, and midrapidity transverse-energy distributions, $dE_T/d\eta$, are presented for a variety of collision systems and energies. Included are distributions for Au+Au collisions at $\sqrt{s_{NN}}$ = 200, 130, 62.4, 39, 27,19.6, 14.5, and 7.7 GeV, Cu+Cu collisions at $\sqrt{s_{NN}}$ = 200 and 62.4 GeV, Cu+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV, U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV, d+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV, $^3$He+Au collisions at $\sqrt{s_{NN}}$ 200 GeV, and p+p collisions at $\sqrt{s_{NN}}$ = 200 GeV. Centrality dependent distributions at midrapidity are presented in terms of the number of nucleon participants, Npart, and the number of constituent quark participants, $N_{qp}$. For all A+A collisions down to $\sqrt{s_{NN}}$ = 7.7 GeV, it is observed that the midrapidity data are better described by scaling with $N_{qp}$ than scaling with $N_{part}$. Also presented are estimates of the Bjorken energy density, $\epsilon_{BJ}$, and the ratio of $dET/d\eta$ to $dNch/d\eta$, the latter of which is seen to be constant as a function of centrality for all systems.
DOI: 10.17182/hepdata.96601.v1/t8
title: "Table 14" of "Transverse energy production and charged-particle multiplicity at midrapidity in various systems from $\sqrt{s_{NN}}=7.7$ to 200 GeV"

description: Multiplicity in Au+Au collisions at $\sqrt{s_{NN}}$ = 39 GeV
description: BNL-RHIC. Measurements of midrapidity charged particle multiplicity distributions, $dN_{ch}/d\eta$, and midrapidity transverse-energy distributions, $dE_T/d\eta$, are presented for a variety of collision systems and energies. Included are distributions for Au+Au collisions at $\sqrt{s_{NN}}$ = 200, 130, 62.4, 39, 27,19.6, 14.5, and 7.7 GeV, Cu+Cu collisions at $\sqrt{s_{NN}}$ = 200 and 62.4 GeV, Cu+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV, U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV, d+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV, $^3$He+Au collisions at $\sqrt{s_{NN}}$ 200 GeV, and p+p collisions at $\sqrt{s_{NN}}$ = 200 GeV. Centrality dependent distributions at midrapidity are presented in terms of the number of nucleon participants, Npart, and the number of constituent quark participants, $N_{qp}$. For all A+A collisions down to $\sqrt{s_{NN}}$ = 7.7 GeV, it is observed that the midrapidity data are better described by scaling with $N_{qp}$ than scaling with $N_{part}$. Also presented are estimates of the Bjorken energy density, $\epsilon_{BJ}$, and the ratio of $dET/d\eta$ to $dNch/d\eta$, the latter of which is seen to be constant as a function of centrality for all systems.
DOI: 10.17182/hepdata.96601.v1/t9
title: "Table 15" of "Transverse energy production and charged-particle multiplicity at midrapidity in various systems from $\sqrt{s_{NN}}=7.7$ to 200 GeV"

description: Transverse energy in Au+Au collisions at $\sqrt{s_{NN}}$ = 27 GeV
description: BNL-RHIC. Measurements of midrapidity charged particle multiplicity distributions, $dN_{ch}/d\eta$, and midrapidity transverse-energy distributions, $dE_T/d\eta$, are presented for a variety of collision systems and energies. Included are distributions for Au+Au collisions at $\sqrt{s_{NN}}$ = 200, 130, 62.4, 39, 27,19.6, 14.5, and 7.7 GeV, Cu+Cu collisions at $\sqrt{s_{NN}}$ = 200 and 62.4 GeV, Cu+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV, U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV, d+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV, $^3$He+Au collisions at $\sqrt{s_{NN}}$ 200 GeV, and p+p collisions at $\sqrt{s_{NN}}$ = 200 GeV. Centrality dependent distributions at midrapidity are presented in terms of the number of nucleon participants, Npart, and the number of constituent quark participants, $N_{qp}$. For all A+A collisions down to $\sqrt{s_{NN}}$ = 7.7 GeV, it is observed that the midrapidity data are better described by scaling with $N_{qp}$ than scaling with $N_{part}$. Also presented are estimates of the Bjorken energy density, $\epsilon_{BJ}$, and the ratio of $dET/d\eta$ to $dNch/d\eta$, the latter of which is seen to be constant as a function of centrality for all systems.
DOI: 10.3535/5df-4jw-3z8
title: Calluna vulgaris (L.) Hull

description: Digital Specimen for the physical specimen hosted at Botanic Garden and Botanical Museum Berlin.
DOI: 10.3535/saw-a88-w3g
title: Salix cinerea L.

description: Digital Specimen for the physical specimen hosted at Botanic Garden and Botanical Museum Berlin.
DOI: 10.17182/hepdata.96601.v1/t14
title: "Table 20" of "Transverse energy production and charged-particle multiplicity at midrapidity in various systems from $\sqrt{s_{NN}}=7.7$ to 200 GeV"

description: Multiplicity in Au+Au collisions at $\sqrt{s_{NN}}$ = 14.5 GeV
description: BNL-RHIC. Measurements of midrapidity charged particle multiplicity distributions, $dN_{ch}/d\eta$, and midrapidity transverse-energy distributions, $dE_T/d\eta$, are presented for a variety of collision systems and energies. Included are distributions for Au+Au collisions at $\sqrt{s_{NN}}$ = 200, 130, 62.4, 39, 27,19.6, 14.5, and 7.7 GeV, Cu+Cu collisions at $\sqrt{s_{NN}}$ = 200 and 62.4 GeV, Cu+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV, U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV, d+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV, $^3$He+Au collisions at $\sqrt{s_{NN}}$ 200 GeV, and p+p collisions at $\sqrt{s_{NN}}$ = 200 GeV. Centrality dependent distributions at midrapidity are presented in terms of the number of nucleon participants, Npart, and the number of constituent quark participants, $N_{qp}$. For all A+A collisions down to $\sqrt{s_{NN}}$ = 7.7 GeV, it is observed that the midrapidity data are better described by scaling with $N_{qp}$ than scaling with $N_{part}$. Also presented are estimates of the Bjorken energy density, $\epsilon_{BJ}$, and the ratio of $dET/d\eta$ to $dNch/d\eta$, the latter of which is seen to be constant as a function of centrality for all systems.
DOI: 10.17182/hepdata.96601.v1/t15
title: "Table 21" of "Transverse energy production and charged-particle multiplicity at midrapidity in various systems from $\sqrt{s_{NN}}=7.7$ to 200 GeV"

description: Transverse energy in Au+Au collisions at $\sqrt{s_{NN}}$ = 7.7 GeV
description: BNL-RHIC. Measurements of midrapidity charged particle multiplicity distributions, $dN_{ch}/d\eta$, and midrapidity transverse-energy distributions, $dE_T/d\eta$, are presented for a variety of collision systems and energies. Included are distributions for Au+Au collisions at $\sqrt{s_{NN}}$ = 200, 130, 62.4, 39, 27,19.6, 14.5, and 7.7 GeV, Cu+Cu collisions at $\sqrt{s_{NN}}$ = 200 and 62.4 GeV, Cu+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV, U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV, d+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV, $^3$He+Au collisions at $\sqrt{s_{NN}}$ 200 GeV, and p+p collisions at $\sqrt{s_{NN}}$ = 200 GeV. Centrality dependent distributions at midrapidity are presented in terms of the number of nucleon participants, Npart, and the number of constituent quark participants, $N_{qp}$. For all A+A collisions down to $\sqrt{s_{NN}}$ = 7.7 GeV, it is observed that the midrapidity data are better described by scaling with $N_{qp}$ than scaling with $N_{part}$. Also presented are estimates of the Bjorken energy density, $\epsilon_{BJ}$, and the ratio of $dET/d\eta$ to $dNch/d\eta$, the latter of which is seen to be constant as a function of centrality for all systems.
DOI: 10.17182/hepdata.96601.v1/t16
title: "Table 22" of "Transverse energy production and charged-particle multiplicity at midrapidity in various systems from $\sqrt{s_{NN}}=7.7$ to 200 GeV"

description: Multiplicity in Au+Au collisions at $\sqrt{s_{NN}}$ = 7.7 GeV
description: BNL-RHIC. Measurements of midrapidity charged particle multiplicity distributions, $dN_{ch}/d\eta$, and midrapidity transverse-energy distributions, $dE_T/d\eta$, are presented for a variety of collision systems and energies. Included are distributions for Au+Au collisions at $\sqrt{s_{NN}}$ = 200, 130, 62.4, 39, 27,19.6, 14.5, and 7.7 GeV, Cu+Cu collisions at $\sqrt{s_{NN}}$ = 200 and 62.4 GeV, Cu+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV, U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV, d+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV, $^3$He+Au collisions at $\sqrt{s_{NN}}$ 200 GeV, and p+p collisions at $\sqrt{s_{NN}}$ = 200 GeV. Centrality dependent distributions at midrapidity are presented in terms of the number of nucleon participants, Npart, and the number of constituent quark participants, $N_{qp}$. For all A+A collisions down to $\sqrt{s_{NN}}$ = 7.7 GeV, it is observed that the midrapidity data are better described by scaling with $N_{qp}$ than scaling with $N_{part}$. Also presented are estimates of the Bjorken energy density, $\epsilon_{BJ}$, and the ratio of $dET/d\eta$ to $dNch/d\eta$, the latter of which is seen to be constant as a function of centrality for all systems.
DOI: 10.17182/hepdata.96601.v1/t17
title: "Table 23" of "Transverse energy production and charged-particle multiplicity at midrapidity in various systems from $\sqrt{s_{NN}}=7.7$ to 200 GeV"

description: Transverse energy in Cu+Cu collisions at $\sqrt{s_{NN}}$ = 200 GeV
description: BNL-RHIC. Measurements of midrapidity charged particle multiplicity distributions, $dN_{ch}/d\eta$, and midrapidity transverse-energy distributions, $dE_T/d\eta$, are presented for a variety of collision systems and energies. Included are distributions for Au+Au collisions at $\sqrt{s_{NN}}$ = 200, 130, 62.4, 39, 27,19.6, 14.5, and 7.7 GeV, Cu+Cu collisions at $\sqrt{s_{NN}}$ = 200 and 62.4 GeV, Cu+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV, U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV, d+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV, $^3$He+Au collisions at $\sqrt{s_{NN}}$ 200 GeV, and p+p collisions at $\sqrt{s_{NN}}$ = 200 GeV. Centrality dependent distributions at midrapidity are presented in terms of the number of nucleon participants, Npart, and the number of constituent quark participants, $N_{qp}$. For all A+A collisions down to $\sqrt{s_{NN}}$ = 7.7 GeV, it is observed that the midrapidity data are better described by scaling with $N_{qp}$ than scaling with $N_{part}$. Also presented are estimates of the Bjorken energy density, $\epsilon_{BJ}$, and the ratio of $dET/d\eta$ to $dNch/d\eta$, the latter of which is seen to be constant as a function of centrality for all systems.
DOI: 10.17182/hepdata.96601.v1/t18
title: "Table 24" of "Transverse energy production and charged-particle multiplicity at midrapidity in various systems from $\sqrt{s_{NN}}=7.7$ to 200 GeV"

description: Multiplicity in Cu+Cu collisions at $\sqrt{s_{NN}}$ = 200 GeV
description: BNL-RHIC. Measurements of midrapidity charged particle multiplicity distributions, $dN_{ch}/d\eta$, and midrapidity transverse-energy distributions, $dE_T/d\eta$, are presented for a variety of collision systems and energies. Included are distributions for Au+Au collisions at $\sqrt{s_{NN}}$ = 200, 130, 62.4, 39, 27,19.6, 14.5, and 7.7 GeV, Cu+Cu collisions at $\sqrt{s_{NN}}$ = 200 and 62.4 GeV, Cu+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV, U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV, d+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV, $^3$He+Au collisions at $\sqrt{s_{NN}}$ 200 GeV, and p+p collisions at $\sqrt{s_{NN}}$ = 200 GeV. Centrality dependent distributions at midrapidity are presented in terms of the number of nucleon participants, Npart, and the number of constituent quark participants, $N_{qp}$. For all A+A collisions down to $\sqrt{s_{NN}}$ = 7.7 GeV, it is observed that the midrapidity data are better described by scaling with $N_{qp}$ than scaling with $N_{part}$. Also presented are estimates of the Bjorken energy density, $\epsilon_{BJ}$, and the ratio of $dET/d\eta$ to $dNch/d\eta$, the latter of which is seen to be constant as a function of centrality for all systems.
DOI: 10.17182/hepdata.96601.v1/t19
title: "Table 25" of "Transverse energy production and charged-particle multiplicity at midrapidity in various systems from $\sqrt{s_{NN}}=7.7$ to 200 GeV"

description: Transverse energy in Cu+Cu collisions at $\sqrt{s_{NN}}$ = 62.4 GeV
description: BNL-RHIC. Measurements of midrapidity charged particle multiplicity distributions, $dN_{ch}/d\eta$, and midrapidity transverse-energy distributions, $dE_T/d\eta$, are presented for a variety of collision systems and energies. Included are distributions for Au+Au collisions at $\sqrt{s_{NN}}$ = 200, 130, 62.4, 39, 27,19.6, 14.5, and 7.7 GeV, Cu+Cu collisions at $\sqrt{s_{NN}}$ = 200 and 62.4 GeV, Cu+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV, U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV, d+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV, $^3$He+Au collisions at $\sqrt{s_{NN}}$ 200 GeV, and p+p collisions at $\sqrt{s_{NN}}$ = 200 GeV. Centrality dependent distributions at midrapidity are presented in terms of the number of nucleon participants, Npart, and the number of constituent quark participants, $N_{qp}$. For all A+A collisions down to $\sqrt{s_{NN}}$ = 7.7 GeV, it is observed that the midrapidity data are better described by scaling with $N_{qp}$ than scaling with $N_{part}$. Also presented are estimates of the Bjorken energy density, $\epsilon_{BJ}$, and the ratio of $dET/d\eta$ to $dNch/d\eta$, the latter of which is seen to be constant as a function of centrality for all systems.
DOI: 10.17182/hepdata.96601.v1/t20
title: "Table 26" of "Transverse energy production and charged-particle multiplicity at midrapidity in various systems from $\sqrt{s_{NN}}=7.7$ to 200 GeV"

description: Multiplicity in Cu+Cu collisions at $\sqrt{s_{NN}}$ = 62.4 GeV
description: BNL-RHIC. Measurements of midrapidity charged particle multiplicity distributions, $dN_{ch}/d\eta$, and midrapidity transverse-energy distributions, $dE_T/d\eta$, are presented for a variety of collision systems and energies. Included are distributions for Au+Au collisions at $\sqrt{s_{NN}}$ = 200, 130, 62.4, 39, 27,19.6, 14.5, and 7.7 GeV, Cu+Cu collisions at $\sqrt{s_{NN}}$ = 200 and 62.4 GeV, Cu+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV, U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV, d+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV, $^3$He+Au collisions at $\sqrt{s_{NN}}$ 200 GeV, and p+p collisions at $\sqrt{s_{NN}}$ = 200 GeV. Centrality dependent distributions at midrapidity are presented in terms of the number of nucleon participants, Npart, and the number of constituent quark participants, $N_{qp}$. For all A+A collisions down to $\sqrt{s_{NN}}$ = 7.7 GeV, it is observed that the midrapidity data are better described by scaling with $N_{qp}$ than scaling with $N_{part}$. Also presented are estimates of the Bjorken energy density, $\epsilon_{BJ}$, and the ratio of $dET/d\eta$ to $dNch/d\eta$, the latter of which is seen to be constant as a function of centrality for all systems.
DOI: 10.17182/hepdata.96601.v1/t21
title: "Table 27" of "Transverse energy production and charged-particle multiplicity at midrapidity in various systems from $\sqrt{s_{NN}}=7.7$ to 200 GeV"

description: Transverse energy in Cu+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV
description: BNL-RHIC. Measurements of midrapidity charged particle multiplicity distributions, $dN_{ch}/d\eta$, and midrapidity transverse-energy distributions, $dE_T/d\eta$, are presented for a variety of collision systems and energies. Included are distributions for Au+Au collisions at $\sqrt{s_{NN}}$ = 200, 130, 62.4, 39, 27,19.6, 14.5, and 7.7 GeV, Cu+Cu collisions at $\sqrt{s_{NN}}$ = 200 and 62.4 GeV, Cu+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV, U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV, d+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV, $^3$He+Au collisions at $\sqrt{s_{NN}}$ 200 GeV, and p+p collisions at $\sqrt{s_{NN}}$ = 200 GeV. Centrality dependent distributions at midrapidity are presented in terms of the number of nucleon participants, Npart, and the number of constituent quark participants, $N_{qp}$. For all A+A collisions down to $\sqrt{s_{NN}}$ = 7.7 GeV, it is observed that the midrapidity data are better described by scaling with $N_{qp}$ than scaling with $N_{part}$. Also presented are estimates of the Bjorken energy density, $\epsilon_{BJ}$, and the ratio of $dET/d\eta$ to $dNch/d\eta$, the latter of which is seen to be constant as a function of centrality for all systems.
DOI: 10.17182/hepdata.96601.v1/t22
title: "Table 28" of "Transverse energy production and charged-particle multiplicity at midrapidity in various systems from $\sqrt{s_{NN}}=7.7$ to 200 GeV"

description: Multiplicity in Cu+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV
description: BNL-RHIC. Measurements of midrapidity charged particle multiplicity distributions, $dN_{ch}/d\eta$, and midrapidity transverse-energy distributions, $dE_T/d\eta$, are presented for a variety of collision systems and energies. Included are distributions for Au+Au collisions at $\sqrt{s_{NN}}$ = 200, 130, 62.4, 39, 27,19.6, 14.5, and 7.7 GeV, Cu+Cu collisions at $\sqrt{s_{NN}}$ = 200 and 62.4 GeV, Cu+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV, U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV, d+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV, $^3$He+Au collisions at $\sqrt{s_{NN}}$ 200 GeV, and p+p collisions at $\sqrt{s_{NN}}$ = 200 GeV. Centrality dependent distributions at midrapidity are presented in terms of the number of nucleon participants, Npart, and the number of constituent quark participants, $N_{qp}$. For all A+A collisions down to $\sqrt{s_{NN}}$ = 7.7 GeV, it is observed that the midrapidity data are better described by scaling with $N_{qp}$ than scaling with $N_{part}$. Also presented are estimates of the Bjorken energy density, $\epsilon_{BJ}$, and the ratio of $dET/d\eta$ to $dNch/d\eta$, the latter of which is seen to be constant as a function of centrality for all systems.
DOI: 10.3535/b4v-5h4-jed
title: Quercus rubra L.

description: Digital Specimen for the physical specimen hosted at Botanic Garden and Botanical Museum Berlin.
DOI: 10.3535/p1z-f7n-0fm
title: Koeleria macrantha (Ledeb.) Schult.

description: Digital Specimen for the physical specimen hosted at Botanic Garden and Botanical Museum Berlin.
DOI: 10.17182/hepdata.96601.v1/t23
title: "Table 29" of "Transverse energy production and charged-particle multiplicity at midrapidity in various systems from $\sqrt{s_{NN}}=7.7$ to 200 GeV"

description: Transverse energy in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV
description: BNL-RHIC. Measurements of midrapidity charged particle multiplicity distributions, $dN_{ch}/d\eta$, and midrapidity transverse-energy distributions, $dE_T/d\eta$, are presented for a variety of collision systems and energies. Included are distributions for Au+Au collisions at $\sqrt{s_{NN}}$ = 200, 130, 62.4, 39, 27,19.6, 14.5, and 7.7 GeV, Cu+Cu collisions at $\sqrt{s_{NN}}$ = 200 and 62.4 GeV, Cu+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV, U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV, d+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV, $^3$He+Au collisions at $\sqrt{s_{NN}}$ 200 GeV, and p+p collisions at $\sqrt{s_{NN}}$ = 200 GeV. Centrality dependent distributions at midrapidity are presented in terms of the number of nucleon participants, Npart, and the number of constituent quark participants, $N_{qp}$. For all A+A collisions down to $\sqrt{s_{NN}}$ = 7.7 GeV, it is observed that the midrapidity data are better described by scaling with $N_{qp}$ than scaling with $N_{part}$. Also presented are estimates of the Bjorken energy density, $\epsilon_{BJ}$, and the ratio of $dET/d\eta$ to $dNch/d\eta$, the latter of which is seen to be constant as a function of centrality for all systems.
DOI: 10.17182/hepdata.96601.v1/t24
title: "Table 30" of "Transverse energy production and charged-particle multiplicity at midrapidity in various systems from $\sqrt{s_{NN}}=7.7$ to 200 GeV"

description: Multiplicity in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV
description: BNL-RHIC. Measurements of midrapidity charged particle multiplicity distributions, $dN_{ch}/d\eta$, and midrapidity transverse-energy distributions, $dE_T/d\eta$, are presented for a variety of collision systems and energies. Included are distributions for Au+Au collisions at $\sqrt{s_{NN}}$ = 200, 130, 62.4, 39, 27,19.6, 14.5, and 7.7 GeV, Cu+Cu collisions at $\sqrt{s_{NN}}$ = 200 and 62.4 GeV, Cu+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV, U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV, d+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV, $^3$He+Au collisions at $\sqrt{s_{NN}}$ 200 GeV, and p+p collisions at $\sqrt{s_{NN}}$ = 200 GeV. Centrality dependent distributions at midrapidity are presented in terms of the number of nucleon participants, Npart, and the number of constituent quark participants, $N_{qp}$. For all A+A collisions down to $\sqrt{s_{NN}}$ = 7.7 GeV, it is observed that the midrapidity data are better described by scaling with $N_{qp}$ than scaling with $N_{part}$. Also presented are estimates of the Bjorken energy density, $\epsilon_{BJ}$, and the ratio of $dET/d\eta$ to $dNch/d\eta$, the latter of which is seen to be constant as a function of centrality for all systems.