cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.98930.v1/t3
title: "Figure 6 up" of "Multiplicity and pseudorapidity distributions of charged particles and photons at forward pseudorapidity in Au + Au collisions at s(NN)**(1/2) = 62.4-GeV."

description: (Color Online) Variation of $N_{ch}$ normalized to the number of collisions in the FTPC coverage $(2.9 \leq \eta \leq 3.9)$ and $N_{\gamma}$ normalized to number of collisions, in the PMD coverage $(2.3 \leq \eta \leq 3.7)$ as a function of $N_{coll}$. The lower band shows the uncertainty in the ratio due to uncertainties in $N_{coll}$ calculations.
description: We present the centrality dependent measurement of multiplicity and pseudorapidity distributions of charged particles and photons in Au + Au collisions at $\sqrt{s_{NN}}$ = 62.4 GeV. The charged particles and photons are measured in the pseudorapidity region $2.9 \leq \eta \leq 3.9$ and $2.3 \leq \eta \leq 3.7$, respectively. We have studied the scaling of particle production with the number of participating nucleons and the number of binary collisions. The photon and charged particle production in the measured pseudorapidity range has been shown to be consistent with energy independent limiting fragmentation behavior. The photons are observed to follow a centrality independent limiting fragmentation behavior while for the charged particles it is centrality dependent. We have carried out a comparative study of the pseudorapidity distributions of positively charged hadrons, negatively charged hadrons, photons, pions, net protons in nucleus-nucleus collisions and pseudorapidity distributions from p+p collisions. From these comparisons we conclude that baryons in the inclusive charged particle distribution are responsible for the observed centrality dependence of limiting fragmentation. The mesons are found to follow an energy independent behavior of limiting fragmentation while the behavior of baryons seems to be energy dependent.
DOI: 10.17182/hepdata.98930.v1/t4
title: "Figure 6 down" of "Multiplicity and pseudorapidity distributions of charged particles and photons at forward pseudorapidity in Au + Au collisions at s(NN)**(1/2) = 62.4-GeV."

description: (Color Online) Variation of $N_{ch}$ normalized to the number of collisions in the FTPC coverage $(2.9 \leq \eta \leq 3.9)$ and $N_{\gamma}$ normalized to number of collisions, in the PMD coverage $(2.3 \leq \eta \leq 3.7)$ as a function of $N_{coll}$. The lower band shows the uncertainty in the ratio due to uncertainties in $N_{coll}$ calculations.
description: We present the centrality dependent measurement of multiplicity and pseudorapidity distributions of charged particles and photons in Au + Au collisions at $\sqrt{s_{NN}}$ = 62.4 GeV. The charged particles and photons are measured in the pseudorapidity region $2.9 \leq \eta \leq 3.9$ and $2.3 \leq \eta \leq 3.7$, respectively. We have studied the scaling of particle production with the number of participating nucleons and the number of binary collisions. The photon and charged particle production in the measured pseudorapidity range has been shown to be consistent with energy independent limiting fragmentation behavior. The photons are observed to follow a centrality independent limiting fragmentation behavior while for the charged particles it is centrality dependent. We have carried out a comparative study of the pseudorapidity distributions of positively charged hadrons, negatively charged hadrons, photons, pions, net protons in nucleus-nucleus collisions and pseudorapidity distributions from p+p collisions. From these comparisons we conclude that baryons in the inclusive charged particle distribution are responsible for the observed centrality dependence of limiting fragmentation. The mesons are found to follow an energy independent behavior of limiting fragmentation while the behavior of baryons seems to be energy dependent.
DOI: 10.17182/hepdata.98930.v1/t5
title: "Figure 7 up" of "Multiplicity and pseudorapidity distributions of charged particles and photons at forward pseudorapidity in Au + Au collisions at s(NN)**(1/2) = 62.4-GeV."

description: (Color Online) $dN/d\eta$ for charged particles and photons for Au + Au collisions at $\sqrt{s_{NN}}$ = 62.4 GeV for various event centrality classes.
description: We present the centrality dependent measurement of multiplicity and pseudorapidity distributions of charged particles and photons in Au + Au collisions at $\sqrt{s_{NN}}$ = 62.4 GeV. The charged particles and photons are measured in the pseudorapidity region $2.9 \leq \eta \leq 3.9$ and $2.3 \leq \eta \leq 3.7$, respectively. We have studied the scaling of particle production with the number of participating nucleons and the number of binary collisions. The photon and charged particle production in the measured pseudorapidity range has been shown to be consistent with energy independent limiting fragmentation behavior. The photons are observed to follow a centrality independent limiting fragmentation behavior while for the charged particles it is centrality dependent. We have carried out a comparative study of the pseudorapidity distributions of positively charged hadrons, negatively charged hadrons, photons, pions, net protons in nucleus-nucleus collisions and pseudorapidity distributions from p+p collisions. From these comparisons we conclude that baryons in the inclusive charged particle distribution are responsible for the observed centrality dependence of limiting fragmentation. The mesons are found to follow an energy independent behavior of limiting fragmentation while the behavior of baryons seems to be energy dependent.
DOI: 10.17182/hepdata.98930.v1/t6
title: "Figure 7 down" of "Multiplicity and pseudorapidity distributions of charged particles and photons at forward pseudorapidity in Au + Au collisions at s(NN)**(1/2) = 62.4-GeV."

description: (Color Online) $dN/d\eta$ for charged particles and photons for Au + Au collisions at $\sqrt{s_{NN}}$ = 62.4 GeV for various event centrality classes.
description: We present the centrality dependent measurement of multiplicity and pseudorapidity distributions of charged particles and photons in Au + Au collisions at $\sqrt{s_{NN}}$ = 62.4 GeV. The charged particles and photons are measured in the pseudorapidity region $2.9 \leq \eta \leq 3.9$ and $2.3 \leq \eta \leq 3.7$, respectively. We have studied the scaling of particle production with the number of participating nucleons and the number of binary collisions. The photon and charged particle production in the measured pseudorapidity range has been shown to be consistent with energy independent limiting fragmentation behavior. The photons are observed to follow a centrality independent limiting fragmentation behavior while for the charged particles it is centrality dependent. We have carried out a comparative study of the pseudorapidity distributions of positively charged hadrons, negatively charged hadrons, photons, pions, net protons in nucleus-nucleus collisions and pseudorapidity distributions from p+p collisions. From these comparisons we conclude that baryons in the inclusive charged particle distribution are responsible for the observed centrality dependence of limiting fragmentation. The mesons are found to follow an energy independent behavior of limiting fragmentation while the behavior of baryons seems to be energy dependent.
DOI: 10.17182/hepdata.98930.v1/t7
title: "Figure 10 up" of "Multiplicity and pseudorapidity distributions of charged particles and photons at forward pseudorapidity in Au + Au collisions at s(NN)**(1/2) = 62.4-GeV."

description: (Color Online) Half width at half maximum of the pseudorapidity distributions ($\eta_{h}$) of charged particles as a function of total charged particle multiplicity ($N_{T}$) normalized to the center of mass energy. The Au + Au collision data are from the PHOBOS [8] experiment and p + p collision data are from the ISR [31] experiments.
description: We present the centrality dependent measurement of multiplicity and pseudorapidity distributions of charged particles and photons in Au + Au collisions at $\sqrt{s_{NN}}$ = 62.4 GeV. The charged particles and photons are measured in the pseudorapidity region $2.9 \leq \eta \leq 3.9$ and $2.3 \leq \eta \leq 3.7$, respectively. We have studied the scaling of particle production with the number of participating nucleons and the number of binary collisions. The photon and charged particle production in the measured pseudorapidity range has been shown to be consistent with energy independent limiting fragmentation behavior. The photons are observed to follow a centrality independent limiting fragmentation behavior while for the charged particles it is centrality dependent. We have carried out a comparative study of the pseudorapidity distributions of positively charged hadrons, negatively charged hadrons, photons, pions, net protons in nucleus-nucleus collisions and pseudorapidity distributions from p+p collisions. From these comparisons we conclude that baryons in the inclusive charged particle distribution are responsible for the observed centrality dependence of limiting fragmentation. The mesons are found to follow an energy independent behavior of limiting fragmentation while the behavior of baryons seems to be energy dependent.
DOI: 10.17182/hepdata.98930.v1/t8
title: "Figure 10 down" of "Multiplicity and pseudorapidity distributions of charged particles and photons at forward pseudorapidity in Au + Au collisions at s(NN)**(1/2) = 62.4-GeV."

description: (Color Online) Half width at half maximum of the pseudorapidity distributions ($\eta_{h}$) of charged particles as a function of total charged particle multiplicity ($N_{T}$) normalized to the center of mass energy. The Au + Au collision data are from the PHOBOS [8] experiment and p + p collision data are from the ISR [31] experiments.
description: We present the centrality dependent measurement of multiplicity and pseudorapidity distributions of charged particles and photons in Au + Au collisions at $\sqrt{s_{NN}}$ = 62.4 GeV. The charged particles and photons are measured in the pseudorapidity region $2.9 \leq \eta \leq 3.9$ and $2.3 \leq \eta \leq 3.7$, respectively. We have studied the scaling of particle production with the number of participating nucleons and the number of binary collisions. The photon and charged particle production in the measured pseudorapidity range has been shown to be consistent with energy independent limiting fragmentation behavior. The photons are observed to follow a centrality independent limiting fragmentation behavior while for the charged particles it is centrality dependent. We have carried out a comparative study of the pseudorapidity distributions of positively charged hadrons, negatively charged hadrons, photons, pions, net protons in nucleus-nucleus collisions and pseudorapidity distributions from p+p collisions. From these comparisons we conclude that baryons in the inclusive charged particle distribution are responsible for the observed centrality dependence of limiting fragmentation. The mesons are found to follow an energy independent behavior of limiting fragmentation while the behavior of baryons seems to be energy dependent.
DOI: 10.17182/hepdata.98930.v1/t9
title: "Figure 15" of "Multiplicity and pseudorapidity distributions of charged particles and photons at forward pseudorapidity in Au + Au collisions at s(NN)**(1/2) = 62.4-GeV."

description: (Color Online) Variation of $dN_{ch}/d\eta$ normalized to $N_{part}$ with $\eta – y_{beam}$ for central and peripheral collisions for positively charged hadrons ($h^{+}$) and negatively charged hadrons ($h^{−}$).
description: We present the centrality dependent measurement of multiplicity and pseudorapidity distributions of charged particles and photons in Au + Au collisions at $\sqrt{s_{NN}}$ = 62.4 GeV. The charged particles and photons are measured in the pseudorapidity region $2.9 \leq \eta \leq 3.9$ and $2.3 \leq \eta \leq 3.7$, respectively. We have studied the scaling of particle production with the number of participating nucleons and the number of binary collisions. The photon and charged particle production in the measured pseudorapidity range has been shown to be consistent with energy independent limiting fragmentation behavior. The photons are observed to follow a centrality independent limiting fragmentation behavior while for the charged particles it is centrality dependent. We have carried out a comparative study of the pseudorapidity distributions of positively charged hadrons, negatively charged hadrons, photons, pions, net protons in nucleus-nucleus collisions and pseudorapidity distributions from p+p collisions. From these comparisons we conclude that baryons in the inclusive charged particle distribution are responsible for the observed centrality dependence of limiting fragmentation. The mesons are found to follow an energy independent behavior of limiting fragmentation while the behavior of baryons seems to be energy dependent.
DOI: 10.25549/vercoutere-ouc110610674
title: Prone nude woman in red and white

description: One nude female outlined in blue and painted red and white lying on a black background. See description of 001 for OT notes.
DOI: 10.3535/kgv-8dg-rt0
title: Trichosanthes L.

description: Digital Specimen for the physical specimen hosted at Botanic Garden and Botanical Museum Berlin.
DOI: 10.3535/mcp-070-hxl
title: Melastoma L.

description: Digital Specimen for the physical specimen hosted at Botanic Garden and Botanical Museum Berlin.
DOI: 10.17182/hepdata.98930.v1/t10
title: "Figure 17 up" of "Multiplicity and pseudorapidity distributions of charged particles and photons at forward pseudorapidity in Au + Au collisions at s(NN)**(1/2) = 62.4-GeV."

description: (Color Online) The top panel shows the variation of pion rapidity density normalized to $N_{part}$ with $y – y_{beam}$ for central collisions at various collision energies. Also shown is the estimated $dN_{\pi^{0}}/dy$ obtained from $dN\_{\gamma}/dy$ normalized to $N_{part}$. The bottom panel shows the variation of net proton rapidity density normalized to $N_{part}$ with $y – y_{beam}$ for central collisions at various collision energies.
description: We present the centrality dependent measurement of multiplicity and pseudorapidity distributions of charged particles and photons in Au + Au collisions at $\sqrt{s_{NN}}$ = 62.4 GeV. The charged particles and photons are measured in the pseudorapidity region $2.9 \leq \eta \leq 3.9$ and $2.3 \leq \eta \leq 3.7$, respectively. We have studied the scaling of particle production with the number of participating nucleons and the number of binary collisions. The photon and charged particle production in the measured pseudorapidity range has been shown to be consistent with energy independent limiting fragmentation behavior. The photons are observed to follow a centrality independent limiting fragmentation behavior while for the charged particles it is centrality dependent. We have carried out a comparative study of the pseudorapidity distributions of positively charged hadrons, negatively charged hadrons, photons, pions, net protons in nucleus-nucleus collisions and pseudorapidity distributions from p+p collisions. From these comparisons we conclude that baryons in the inclusive charged particle distribution are responsible for the observed centrality dependence of limiting fragmentation. The mesons are found to follow an energy independent behavior of limiting fragmentation while the behavior of baryons seems to be energy dependent.
DOI: 10.17182/hepdata.98930.v1/t11
title: "Figure 17 down" of "Multiplicity and pseudorapidity distributions of charged particles and photons at forward pseudorapidity in Au + Au collisions at s(NN)**(1/2) = 62.4-GeV."

description: (Color Online) The top panel shows the variation of pion rapidity density normalized to $N_{part}$ with $y – y_{beam}$ for central collisions at various collision energies. Also shown is the estimated $dN_{\pi^{0}}/dy$ obtained from $dN\_{\gamma}/dy$ normalized to $N_{part}$. The bottom panel shows the variation of net proton rapidity density normalized to $N_{part}$ with $y – y_{beam}$ for central collisions at various collision energies.
description: We present the centrality dependent measurement of multiplicity and pseudorapidity distributions of charged particles and photons in Au + Au collisions at $\sqrt{s_{NN}}$ = 62.4 GeV. The charged particles and photons are measured in the pseudorapidity region $2.9 \leq \eta \leq 3.9$ and $2.3 \leq \eta \leq 3.7$, respectively. We have studied the scaling of particle production with the number of participating nucleons and the number of binary collisions. The photon and charged particle production in the measured pseudorapidity range has been shown to be consistent with energy independent limiting fragmentation behavior. The photons are observed to follow a centrality independent limiting fragmentation behavior while for the charged particles it is centrality dependent. We have carried out a comparative study of the pseudorapidity distributions of positively charged hadrons, negatively charged hadrons, photons, pions, net protons in nucleus-nucleus collisions and pseudorapidity distributions from p+p collisions. From these comparisons we conclude that baryons in the inclusive charged particle distribution are responsible for the observed centrality dependence of limiting fragmentation. The mesons are found to follow an energy independent behavior of limiting fragmentation while the behavior of baryons seems to be energy dependent.
DOI: 10.17182/hepdata.98931.v1/t1
title: "Figure 2 up" of "Measurement of the $W \to e \nu$ and $Z/\gamma^* \to e^+e^-$ Production Cross Sections at Mid-rapidity in Proton-Proton Collisions at $\sqrt{s}$ = 500 GeV"

description: (Color online) Trigger rate as a function of vernier scan beam displacement in the x and y directions. The transverse beam widths ($\sigma_{x}$ and $\sigma_{y}$) and maximum trigger rate ($R^{max}_{ver}$) were extracted from the fit, which is superimposed.
description: We report measurements of the charge-separated $W^{+(−)} \to e^{+(−)} + \nu_{e}(\overline{\nu}_{e})$ and $Z/\gamma^{*} \to e^{+}e^{−}$ production cross sections at mid-rapidity in proton-proton collisions at $\sqrt{s}$ = 500 GeV. These results are based on 13.2 $pb^{−1}$ of data recorded in 2009 by the STAR detector at RHIC. Production cross sections for W bosons that decay via the $e\nu$ channel were measured to be $\sigma(pp \to W^{+}X)·BR(W^{+} \to e^{+} \nu_{e})$ = 117.3 $\pm$ 5.9(stat) $\pm$ 6.2(syst) $\pm$ 15.2(lumi) pb, and $\sigma(pp \to W^{−}X)·BR(W^{−} \to e^{−}\overline{\nu}_{e})$ = 43.3 $\pm$ 4.6(stat) $\pm$ 3.4(syst) $\pm$ 5.6(lumi) pb. For $Z/\gamma^{*}$ production, $\sigma(pp \to Z/\gamma^{∗} X) · BR(Z/\gamma^{*} \to e^{+}e^{−})$ = 7.7 $\pm$ 2.1(stat) ${}^{+0.5}_{-0.9}$(syst) $\pm$ 1.0(lumi) pb for di-lepton invariant masses $m_{e^{+}e^{-}}$ between 70 and 110 GeV/$c^{2}$. First measurements of the W cross section ratio, $\sigma(pp \to W^{+}X)/\sigma(pp \to W^{-}X)$, at $\sqrt{s}$ = 500 GeV are also reported. Theoretical predictions, calculated using recent parton distribution functions, are found to agree with the measured cross sections.
DOI: 10.17182/hepdata.98931.v1/t2
title: "Figure 2 down" of "Measurement of the $W \to e \nu$ and $Z/\gamma^* \to e^+e^-$ Production Cross Sections at Mid-rapidity in Proton-Proton Collisions at $\sqrt{s}$ = 500 GeV"

description: (Color online) Trigger rate as a function of vernier scan beam displacement in the x and y directions. The transverse beam widths ($\sigma_{x}$ and $\sigma_{y}$) and maximum trigger rate ($R^{max}_{ver}$) were extracted from the fit, which is superimposed.
description: We report measurements of the charge-separated $W^{+(−)} \to e^{+(−)} + \nu_{e}(\overline{\nu}_{e})$ and $Z/\gamma^{*} \to e^{+}e^{−}$ production cross sections at mid-rapidity in proton-proton collisions at $\sqrt{s}$ = 500 GeV. These results are based on 13.2 $pb^{−1}$ of data recorded in 2009 by the STAR detector at RHIC. Production cross sections for W bosons that decay via the $e\nu$ channel were measured to be $\sigma(pp \to W^{+}X)·BR(W^{+} \to e^{+} \nu_{e})$ = 117.3 $\pm$ 5.9(stat) $\pm$ 6.2(syst) $\pm$ 15.2(lumi) pb, and $\sigma(pp \to W^{−}X)·BR(W^{−} \to e^{−}\overline{\nu}_{e})$ = 43.3 $\pm$ 4.6(stat) $\pm$ 3.4(syst) $\pm$ 5.6(lumi) pb. For $Z/\gamma^{*}$ production, $\sigma(pp \to Z/\gamma^{∗} X) · BR(Z/\gamma^{*} \to e^{+}e^{−})$ = 7.7 $\pm$ 2.1(stat) ${}^{+0.5}_{-0.9}$(syst) $\pm$ 1.0(lumi) pb for di-lepton invariant masses $m_{e^{+}e^{-}}$ between 70 and 110 GeV/$c^{2}$. First measurements of the W cross section ratio, $\sigma(pp \to W^{+}X)/\sigma(pp \to W^{-}X)$, at $\sqrt{s}$ = 500 GeV are also reported. Theoretical predictions, calculated using recent parton distribution functions, are found to agree with the measured cross sections.
DOI: 10.17182/hepdata.98931.v1/t3
title: "Figure 5" of "Measurement of the $W \to e \nu$ and $Z/\gamma^* \to e^+e^-$ Production Cross Sections at Mid-rapidity in Proton-Proton Collisions at $\sqrt{s}$ = 500 GeV"

description: (Color online) Distributions of $E^{e}_{T}$ for W candidate events after sequentially applying the selection criteria de- scribed in Secs. IV A and IV B.
description: We report measurements of the charge-separated $W^{+(−)} \to e^{+(−)} + \nu_{e}(\overline{\nu}_{e})$ and $Z/\gamma^{*} \to e^{+}e^{−}$ production cross sections at mid-rapidity in proton-proton collisions at $\sqrt{s}$ = 500 GeV. These results are based on 13.2 $pb^{−1}$ of data recorded in 2009 by the STAR detector at RHIC. Production cross sections for W bosons that decay via the $e\nu$ channel were measured to be $\sigma(pp \to W^{+}X)·BR(W^{+} \to e^{+} \nu_{e})$ = 117.3 $\pm$ 5.9(stat) $\pm$ 6.2(syst) $\pm$ 15.2(lumi) pb, and $\sigma(pp \to W^{−}X)·BR(W^{−} \to e^{−}\overline{\nu}_{e})$ = 43.3 $\pm$ 4.6(stat) $\pm$ 3.4(syst) $\pm$ 5.6(lumi) pb. For $Z/\gamma^{*}$ production, $\sigma(pp \to Z/\gamma^{∗} X) · BR(Z/\gamma^{*} \to e^{+}e^{−})$ = 7.7 $\pm$ 2.1(stat) ${}^{+0.5}_{-0.9}$(syst) $\pm$ 1.0(lumi) pb for di-lepton invariant masses $m_{e^{+}e^{-}}$ between 70 and 110 GeV/$c^{2}$. First measurements of the W cross section ratio, $\sigma(pp \to W^{+}X)/\sigma(pp \to W^{-}X)$, at $\sqrt{s}$ = 500 GeV are also reported. Theoretical predictions, calculated using recent parton distribution functions, are found to agree with the measured cross sections.
DOI: 10.17182/hepdata.98931.v1/t4
title: "Figure 6" of "Measurement of the $W \to e \nu$ and $Z/\gamma^* \to e^+e^-$ Production Cross Sections at Mid-rapidity in Proton-Proton Collisions at $\sqrt{s}$ = 500 GeV"

description: (Color online) Distribution of the product of the TPC reconstructed charge sign and 1/$p_{T}$ for candidates satisfying all the W signal selection criteria and $E^{e}_{T}$ &gt; 25 GeV.
description: We report measurements of the charge-separated $W^{+(−)} \to e^{+(−)} + \nu_{e}(\overline{\nu}_{e})$ and $Z/\gamma^{*} \to e^{+}e^{−}$ production cross sections at mid-rapidity in proton-proton collisions at $\sqrt{s}$ = 500 GeV. These results are based on 13.2 $pb^{−1}$ of data recorded in 2009 by the STAR detector at RHIC. Production cross sections for W bosons that decay via the $e\nu$ channel were measured to be $\sigma(pp \to W^{+}X)·BR(W^{+} \to e^{+} \nu_{e})$ = 117.3 $\pm$ 5.9(stat) $\pm$ 6.2(syst) $\pm$ 15.2(lumi) pb, and $\sigma(pp \to W^{−}X)·BR(W^{−} \to e^{−}\overline{\nu}_{e})$ = 43.3 $\pm$ 4.6(stat) $\pm$ 3.4(syst) $\pm$ 5.6(lumi) pb. For $Z/\gamma^{*}$ production, $\sigma(pp \to Z/\gamma^{∗} X) · BR(Z/\gamma^{*} \to e^{+}e^{−})$ = 7.7 $\pm$ 2.1(stat) ${}^{+0.5}_{-0.9}$(syst) $\pm$ 1.0(lumi) pb for di-lepton invariant masses $m_{e^{+}e^{-}}$ between 70 and 110 GeV/$c^{2}$. First measurements of the W cross section ratio, $\sigma(pp \to W^{+}X)/\sigma(pp \to W^{-}X)$, at $\sqrt{s}$ = 500 GeV are also reported. Theoretical predictions, calculated using recent parton distribution functions, are found to agree with the measured cross sections.
DOI: 10.3535/lr5-0kc-dp0
title: Polygala tonkinensis Chodat

description: Digital Specimen for the physical specimen hosted at Botanic Garden and Botanical Museum Berlin.