cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.99048.v2/t1
title: "Table (a) from Figure 3" of "Longitudinal Spin Transfer to $\Lambda$ and $\bar{\Lambda}$ Hyperons in Polarized Proton-Proton Collisions at $\sqrt{s}$ = 200 GeV"

description: The spin transfer $D_{LL}$ to (a) $\Lambda$ and (b) $\bar{\Lambda}$ hyperons produced at positive pseudorapidity with respect to the polarized proton beam from $MB$, $JP$, and $HT$ data versus hyperon transverse momenta $p_{T}$. The sizes of the statistical and systematic uncertainties are indicated by the vertical bars and bands, respectively. For clarity, the HT data points have been shifted slightly in $p_{T}$. The dotted vertical lines indicate the $p_{T}$ intervals in the analysis of HT and JP data.
description: BNL-RHIC. The longitudinal spin transfer, $D_{LL}$, from high energy polarized protons to $\Lambda$ and $\bar{\Lambda}$ hyperons has been measured for the first time in proton-proton collisions at $\sqrt{s} = 200$ GeV with the STAR detector at the Relativistic Heavy Ion Collider. The measurements cover pseudorapidity, $\eta$, in the range $|\eta| &lt; 1.2$ and transverse momenta, $p_{T}$, up to 4 GeV/c. The longitudinal spin transfer is found to be $D_{LL} = -0.03 \pm 0.13(stat) \pm 0.04(syst)$ for inclusive $\Lambda$ and $D_{LL} = -0.12 \pm 0.08(stat) \pm 0.03(syst)$ for inclusive $\bar{\Lambda}$ hyperons with $&lt;\eta&gt;$ and $ = 3.7 GeV/c$. The dependence on $\eta$ and $p_{T}$ is presented. ***Updated $D_{LL}$ values using the new $\alpha_\Lambda=0.732$ published on PDG2020 are also presented in this HEPData entry.***
DOI: 10.17182/hepdata.99048.v2/t2
title: "Table (b) from Figure 3" of "Longitudinal Spin Transfer to $\Lambda$ and $\bar{\Lambda}$ Hyperons in Polarized Proton-Proton Collisions at $\sqrt{s}$ = 200 GeV"

description: The spin transfer $D_{LL}$ to (a) $\Lambda$ and (b) $\bar{\Lambda}$ hyperons produced at positive pseudorapidity with respect to the polarized proton beam from $MB$, $JP$, and $HT$ data versus hyperon transverse momenta $p_{T}$. The sizes of the statistical and systematic uncertainties are indicated by the vertical bars and bands, respectively. For clarity, the HT data points have been shifted slightly in $p_{T}$. The dotted vertical lines indicate the $p_{T}$ intervals in the analysis of HT and JP data.
description: BNL-RHIC. The longitudinal spin transfer, $D_{LL}$, from high energy polarized protons to $\Lambda$ and $\bar{\Lambda}$ hyperons has been measured for the first time in proton-proton collisions at $\sqrt{s} = 200$ GeV with the STAR detector at the Relativistic Heavy Ion Collider. The measurements cover pseudorapidity, $\eta$, in the range $|\eta| &lt; 1.2$ and transverse momenta, $p_{T}$, up to 4 GeV/c. The longitudinal spin transfer is found to be $D_{LL} = -0.03 \pm 0.13(stat) \pm 0.04(syst)$ for inclusive $\Lambda$ and $D_{LL} = -0.12 \pm 0.08(stat) \pm 0.03(syst)$ for inclusive $\bar{\Lambda}$ hyperons with $&lt;\eta&gt;$ and $ = 3.7 GeV/c$. The dependence on $\eta$ and $p_{T}$ is presented. ***Updated $D_{LL}$ values using the new $\alpha_\Lambda=0.732$ published on PDG2020 are also presented in this HEPData entry.***
DOI: 10.17182/hepdata.99048.v2/t3
title: "Table from Figure 4" of "Longitudinal Spin Transfer to $\Lambda$ and $\bar{\Lambda}$ Hyperons in Polarized Proton-Proton Collisions at $\sqrt{s}$ = 200 GeV"

description: Comparison of $\Lambda$ and $\bar{\Lambda}$ spin transfer $D_{LL}$ in polarized proton-proton collisions at $\sqrt{s} = 200$ GeV for (a) positive and (b) negative $\eta$ versus $p_{T}$. The vertical bars and bands indicate the sizes of the statistical and systematic uncertainties, respectively. The $\bar{\Lambda}$ data points have been shifted slightly in $p_{T}$ for clarity. The dotted vertical lines indicate the $p_{T}$ intervals in the analysis of HT and JP data. The horizontal lines show model predictions evaluated at $\eta$ and largest $p_{T}$ of the data.
description: BNL-RHIC. The longitudinal spin transfer, $D_{LL}$, from high energy polarized protons to $\Lambda$ and $\bar{\Lambda}$ hyperons has been measured for the first time in proton-proton collisions at $\sqrt{s} = 200$ GeV with the STAR detector at the Relativistic Heavy Ion Collider. The measurements cover pseudorapidity, $\eta$, in the range $|\eta| &lt; 1.2$ and transverse momenta, $p_{T}$, up to 4 GeV/c. The longitudinal spin transfer is found to be $D_{LL} = -0.03 \pm 0.13(stat) \pm 0.04(syst)$ for inclusive $\Lambda$ and $D_{LL} = -0.12 \pm 0.08(stat) \pm 0.03(syst)$ for inclusive $\bar{\Lambda}$ hyperons with $&lt;\eta&gt;$ and $ = 3.7 GeV/c$. The dependence on $\eta$ and $p_{T}$ is presented. ***Updated $D_{LL}$ values using the new $\alpha_\Lambda=0.732$ published on PDG2020 are also presented in this HEPData entry.***
DOI: 10.3535/bxj-f7k-mm7
title: Fabaceae

description: Digital Specimen for the physical specimen hosted at Botanic Garden and Botanical Museum Berlin.
DOI: 10.3535/ew0-qva-vxs
title: Rhodomyrtus tomentosa (Aiton) Hassk.

description: Digital Specimen for the physical specimen hosted at Botanic Garden and Botanical Museum Berlin.
DOI: 10.17182/hepdata.99048.v1/t1
title: "Table (a) from Figure 3" of "Longitudinal Spin Transfer to $\Lambda$ and $\bar{\Lambda}$ Hyperons in Polarized Proton-Proton Collisions at $\sqrt{s}$ = 200 GeV"

description: The spin transfer $D_{LL}$ to (a) $\Lambda$ and (b) $\bar{\Lambda}$ hyperons produced at positive pseudorapidity with respect to the polarized proton beam from $MB$, $JP$, and $HT$ data versus hyperon transverse momenta $p_{T}$. The sizes of the statistical and systematic uncertainties are indicated by the vertical bars and bands, respectively. For clarity, the HT data points have been shifted slightly in $p_{T}$. The dotted vertical lines indicate the $p_{T}$ intervals in the analysis of HT and JP data.
description: BNL-RHIC. The longitudinal spin transfer, $D_{LL}$, from high energy polarized protons to $\Lambda$ and $\bar{\Lambda}$ hyperons has been measured for the first time in proton-proton collisions at $\sqrt{s} = 200$ GeV with the STAR detector at the Relativistic Heavy Ion Collider. The measurements cover pseudorapidity, $\eta$, in the range $|\eta| &lt; 1.2$ and transverse momenta, $p_{T}$, up to 4 GeV/c. The longitudinal spin transfer is found to be $D_{LL} = -0.03 \pm 0.13(stat) \pm 0.04(syst)$ for inclusive $\Lambda$ and $D_{LL} = -0.12 \pm 0.08(stat) \pm 0.03(syst)$ for inclusive $\bar{\Lambda}$ hyperons with $&lt;\eta&gt;$ and $ = 3.7 GeV/c$. The dependence on $\eta$ and $p_{T}$ is presented.
DOI: 10.17182/hepdata.99048.v1/t2
title: "Table (b) from Figure 3" of "Longitudinal Spin Transfer to $\Lambda$ and $\bar{\Lambda}$ Hyperons in Polarized Proton-Proton Collisions at $\sqrt{s}$ = 200 GeV"

description: The spin transfer $D_{LL}$ to (a) $\Lambda$ and (b) $\bar{\Lambda}$ hyperons produced at positive pseudorapidity with respect to the polarized proton beam from $MB$, $JP$, and $HT$ data versus hyperon transverse momenta $p_{T}$. The sizes of the statistical and systematic uncertainties are indicated by the vertical bars and bands, respectively. For clarity, the HT data points have been shifted slightly in $p_{T}$. The dotted vertical lines indicate the $p_{T}$ intervals in the analysis of HT and JP data.
description: BNL-RHIC. The longitudinal spin transfer, $D_{LL}$, from high energy polarized protons to $\Lambda$ and $\bar{\Lambda}$ hyperons has been measured for the first time in proton-proton collisions at $\sqrt{s} = 200$ GeV with the STAR detector at the Relativistic Heavy Ion Collider. The measurements cover pseudorapidity, $\eta$, in the range $|\eta| &lt; 1.2$ and transverse momenta, $p_{T}$, up to 4 GeV/c. The longitudinal spin transfer is found to be $D_{LL} = -0.03 \pm 0.13(stat) \pm 0.04(syst)$ for inclusive $\Lambda$ and $D_{LL} = -0.12 \pm 0.08(stat) \pm 0.03(syst)$ for inclusive $\bar{\Lambda}$ hyperons with $&lt;\eta&gt;$ and $ = 3.7 GeV/c$. The dependence on $\eta$ and $p_{T}$ is presented.
DOI: 10.17182/hepdata.99048.v1/t3
title: "Figure 4" of "Longitudinal Spin Transfer to $\Lambda$ and $\bar{\Lambda}$ Hyperons in Polarized Proton-Proton Collisions at $\sqrt{s}$ = 200 GeV"

description: Comparison of $\Lambda$ and $\bar{\Lambda}$ spin transfer $D_{LL}$ in polarized proton-proton collisions at $\sqrt{s} = 200 GeV$ for (a) positive and (b) negative $\eta$ versus $p_{T}$. The vertical bars and bands indicate the sizes of the statistical and systematic uncertainties, respectively. The $\bar{\Lambda}$ data points have been shifted slightly in $p_{T}$ for clarity. The dotted vertical lines indicate the $p_{T}$ intervals in the analysis of HT and JP data. The horizontal lines show model predictions evaluated at $\eta$ and largest $p_{T}$ of the data.
description: BNL-RHIC. The longitudinal spin transfer, $D_{LL}$, from high energy polarized protons to $\Lambda$ and $\bar{\Lambda}$ hyperons has been measured for the first time in proton-proton collisions at $\sqrt{s} = 200$ GeV with the STAR detector at the Relativistic Heavy Ion Collider. The measurements cover pseudorapidity, $\eta$, in the range $|\eta| &lt; 1.2$ and transverse momenta, $p_{T}$, up to 4 GeV/c. The longitudinal spin transfer is found to be $D_{LL} = -0.03 \pm 0.13(stat) \pm 0.04(syst)$ for inclusive $\Lambda$ and $D_{LL} = -0.12 \pm 0.08(stat) \pm 0.03(syst)$ for inclusive $\bar{\Lambda}$ hyperons with $&lt;\eta&gt;$ and $ = 3.7 GeV/c$. The dependence on $\eta$ and $p_{T}$ is presented.
DOI: 10.17182/hepdata.99048.v2/t4
title: "Table (a) from Figure 3 with New $\alpha$" of "Longitudinal Spin Transfer to $\Lambda$ and $\bar{\Lambda}$ Hyperons in Polarized Proton-Proton Collisions at $\sqrt{s}$ = 200 GeV"

description: The spin transfer $D_{LL}$ to (a) $\Lambda$ and (b) $\bar{\Lambda}$ hyperons, calculated using the new $\alpha_\Lambda=0.732$ updated on PDG2020, produced at positive pseudorapidity with respect to the polarized proton beam from $MB$, $JP$, and $HT$ data versus hyperon transverse momenta $p_{T}$. The sizes of the statistical and systematic uncertainties are indicated by the vertical bars and bands, respectively. For clarity, the HT data points have been shifted slightly in $p_{T}$. The dotted vertical lines indicate the $p_{T}$ intervals in the analysis of HT and JP data.
description: BNL-RHIC. The longitudinal spin transfer, $D_{LL}$, from high energy polarized protons to $\Lambda$ and $\bar{\Lambda}$ hyperons has been measured for the first time in proton-proton collisions at $\sqrt{s} = 200$ GeV with the STAR detector at the Relativistic Heavy Ion Collider. The measurements cover pseudorapidity, $\eta$, in the range $|\eta| &lt; 1.2$ and transverse momenta, $p_{T}$, up to 4 GeV/c. The longitudinal spin transfer is found to be $D_{LL} = -0.03 \pm 0.13(stat) \pm 0.04(syst)$ for inclusive $\Lambda$ and $D_{LL} = -0.12 \pm 0.08(stat) \pm 0.03(syst)$ for inclusive $\bar{\Lambda}$ hyperons with $&lt;\eta&gt;$ and $ = 3.7 GeV/c$. The dependence on $\eta$ and $p_{T}$ is presented. ***Updated $D_{LL}$ values using the new $\alpha_\Lambda=0.732$ published on PDG2020 are also presented in this HEPData entry.***
DOI: 10.17182/hepdata.99048.v2/t5
title: "Table (b) from Figure 3 with New $\alpha$" of "Longitudinal Spin Transfer to $\Lambda$ and $\bar{\Lambda}$ Hyperons in Polarized Proton-Proton Collisions at $\sqrt{s}$ = 200 GeV"

description: The spin transfer $D_{LL}$ to (a) $\Lambda$ and (b) $\bar{\Lambda}$ hyperons, calculated using the new $\alpha_\Lambda=0.732$ updated on PDG2020, produced at positive pseudorapidity with respect to the polarized proton beam from $MB$, $JP$, and $HT$ data versus hyperon transverse momenta $p_{T}$. The sizes of the statistical and systematic uncertainties are indicated by the vertical bars and bands, respectively. For clarity, the HT data points have been shifted slightly in $p_{T}$. The dotted vertical lines indicate the $p_{T}$ intervals in the analysis of HT and JP data.
description: BNL-RHIC. The longitudinal spin transfer, $D_{LL}$, from high energy polarized protons to $\Lambda$ and $\bar{\Lambda}$ hyperons has been measured for the first time in proton-proton collisions at $\sqrt{s} = 200$ GeV with the STAR detector at the Relativistic Heavy Ion Collider. The measurements cover pseudorapidity, $\eta$, in the range $|\eta| &lt; 1.2$ and transverse momenta, $p_{T}$, up to 4 GeV/c. The longitudinal spin transfer is found to be $D_{LL} = -0.03 \pm 0.13(stat) \pm 0.04(syst)$ for inclusive $\Lambda$ and $D_{LL} = -0.12 \pm 0.08(stat) \pm 0.03(syst)$ for inclusive $\bar{\Lambda}$ hyperons with $&lt;\eta&gt;$ and $ = 3.7 GeV/c$. The dependence on $\eta$ and $p_{T}$ is presented. ***Updated $D_{LL}$ values using the new $\alpha_\Lambda=0.732$ published on PDG2020 are also presented in this HEPData entry.***
DOI: 10.17182/hepdata.99048.v2/t6
title: "Table from Figure 4 with New $\alpha$" of "Longitudinal Spin Transfer to $\Lambda$ and $\bar{\Lambda}$ Hyperons in Polarized Proton-Proton Collisions at $\sqrt{s}$ = 200 GeV"

description: Comparison of $\Lambda$ and $\bar{\Lambda}$ spin transfer $D_{LL}$, calculated using the new $\alpha_\Lambda=0.732$ updated on PDG2020, in polarized proton-proton collisions at $\sqrt{s} = 200$ GeV for (a) positive and (b) negative $\eta$ versus $p_{T}$. The vertical bars and bands indicate the sizes of the statistical and systematic uncertainties, respectively. The $\bar{\Lambda}$ data points have been shifted slightly in $p_{T}$ for clarity. The dotted vertical lines indicate the $p_{T}$ intervals in the analysis of HT and JP data. The horizontal lines show model predictions evaluated at $\eta$ and largest $p_{T}$ of the data.
description: BNL-RHIC. The longitudinal spin transfer, $D_{LL}$, from high energy polarized protons to $\Lambda$ and $\bar{\Lambda}$ hyperons has been measured for the first time in proton-proton collisions at $\sqrt{s} = 200$ GeV with the STAR detector at the Relativistic Heavy Ion Collider. The measurements cover pseudorapidity, $\eta$, in the range $|\eta| &lt; 1.2$ and transverse momenta, $p_{T}$, up to 4 GeV/c. The longitudinal spin transfer is found to be $D_{LL} = -0.03 \pm 0.13(stat) \pm 0.04(syst)$ for inclusive $\Lambda$ and $D_{LL} = -0.12 \pm 0.08(stat) \pm 0.03(syst)$ for inclusive $\bar{\Lambda}$ hyperons with $&lt;\eta&gt;$ and $ = 3.7 GeV/c$. The dependence on $\eta$ and $p_{T}$ is presented. ***Updated $D_{LL}$ values using the new $\alpha_\Lambda=0.732$ published on PDG2020 are also presented in this HEPData entry.***
DOI: 10.3535/2bt-5ng-vej
title: Eriocaulon L.

description: Digital Specimen for the physical specimen hosted at Botanic Garden and Botanical Museum Berlin.
DOI: 10.3535/rm8-nng-r9l
title: Anacardiaceae R. Br.

description: Digital Specimen for the physical specimen hosted at Botanic Garden and Botanical Museum Berlin.
DOI: 10.17182/hepdata.99049.v1/t1
title: "Figure 1" of "Multiplicity distribution and spectra of negatively charged hadrons in Au + Au collisions at s(NN)**(1/2) = 130-GeV."

description: Normalized multiplicity distribution of $h^{−}$ with $p_{T} &gt; 100$ MeV/$c$ at $|\eta| &lt; 0.5$ in Au+Au collisions at $\sqrt{s_{NN}} = 130$ GeV. Systematic error on the vertical scale is estimated to be $10\%$. The systematic error on the horizontal scale is $6\%$ for the entire range of multiplicity. The shaded area is $5\%$ most central collisions, selected by ZDC coincidence. The solid curve is the prediction from the HIJING model.
description: No data abstract available.
DOI: 10.17182/hepdata.99049.v1/t2
title: "Figure 2 upper panel" of "Multiplicity distribution and spectra of negatively charged hadrons in Au + Au collisions at s(NN)**(1/2) = 130-GeV."

description: $h^{−}$ $p_{T}$-spectra for the $5\%$ most central Au+Au collisions at midrapidity ($|\eta| &lt; 0.1$) for several systems. The correlated systematical error is estimated to be below $6\%$. The curves are power-law fits to the data.
description: No data abstract available.
DOI: 10.17182/hepdata.99049.v1/t3
title: "Figure 2 lower panel" of "Multiplicity distribution and spectra of negatively charged hadrons in Au + Au collisions at s(NN)**(1/2) = 130-GeV."

description: ratio of STAR and scaled UA1 $p_{T}$-distributions. The errors given are the errors of the STAR data only and do not include the systematic errors from the scaling of the UA1 data to $130$ GeV (i.e., the shaded region in Fig.2 lower panel). The STAR data is for the $5\%$ most central collisions.
description: No data abstract available.
DOI: 10.17182/hepdata.99049.v1/t4
title: "Figure 3" of "Multiplicity distribution and spectra of negatively charged hadrons in Au + Au collisions at s(NN)**(1/2) = 130-GeV."

description: $h^{−}$ pseudorapidity distribution from $5\%$ most central Au+Au collisions for $p_{T} &gt; 100$ MeV/$c$ (filled circles) and all $p_{T}$ (open squares). The correlated systematic error on the overall normalization is estimated to be $6\%$ for $p_{T} &gt; 0.1$ GeV/$c$ and $7\%$ for $p_{T} &gt; 0$.
description: No data abstract available.
DOI: 10.17182/hepdata.99050.v1/t1
title: "Figure 2 left panel" of "Mid-rapidity Lambda and Antilambda production in Au + Au collisions at s(NN)**(1/2) = 130-GeV."

description: Transverse mass distributions of $\Lambda$ at mid-rapidity ($|y|&lt;0.5$) for selected centrality bins. Only statistical errors are listed. Combined systematic errors estimated to be $10\%$. The dashed lines are Boltzmann fits. Note that multiplicative factors have been applied to data from the two most central data sets for display.
description: No data abstract available.
DOI: 10.17182/hepdata.99050.v1/t2
title: "Figure 2 right panel" of "Mid-rapidity Lambda and Antilambda production in Au + Au collisions at s(NN)**(1/2) = 130-GeV."

description: Transverse mass distributions of $\bar\Lambda$ at mid-rapidity ($|y|&lt;0.5$) for selected centrality bins. Only statistical errors are listed. Combined systematic errors estimated to be $10\%$. The dashed lines are Boltzmann fits. Note that multiplicative factors have been applied to data from the two most central data sets for display.
description: No data abstract available.
DOI: 10.17182/hepdata.99050.v1/t3
title: "Figure 3" of "Mid-rapidity Lambda and Antilambda production in Au + Au collisions at s(NN)**(1/2) = 130-GeV."

description: The mid-rapidity $\bar\Lambda$ ($|y|&lt;0.5$) transverse momentum distribution from the top $5\%$ most central collisions. For comparison the distributions for negative hadrons ($d^{2}N/(2 \pi p_{T})dp_{T}d\eta$, $|\eta|&lt;0.1$) and anti-protons ($|y|&lt;0.1$) for the similar centrality bin are included. Only statistical errors are listed. Statistical errors are less than the size of the data points. Combined systematic errors on hyperons estimated to be $10\%$. Correlated systematic errors for negative hadrons estimated to be $6\%$. Systematic errors on antiprotons are $8\%$ point-to-point and $10\%$ in the overall normalization.
description: No data abstract available.
DOI: 10.25549/vercoutere-ouc110610635
title: Headless person sitting on the ground

description: One headless human of undetermined sex depicted in yellow with brown, black, red, orange, and green details sitting on a gray pavement next to orange and black striped floor and a black patterned wall that includes a white anchor against a red and blue background. See description of 001 for OT notes.
DOI: 10.3535/rgg-94v-hlf
title: Scirpus Tourn. ex L.

description: Digital Specimen for the physical specimen hosted at Botanic Garden and Botanical Museum Berlin.
DOI: 10.17182/hepdata.99050.v1/t4
title: "Figure 4" of "Mid-rapidity Lambda and Antilambda production in Au + Au collisions at s(NN)**(1/2) = 130-GeV."

description: $\Lambda$ and $\bar\Lambda$ rapidity density as a function of negative hadron multiplicity at mid-rapidity. The open symbols in the figure are data points from an independent analysis of minimum bias data set using event-mixing techniques. Errors shown are statistical only. Systematic errors on hyperon yields $10\%$, on negative hadron yields $6\%$. $\Lambda$ and $\bar\Lambda$ measured for $|y|&lt;0.5$, negative hadrons for $|\eta|&lt;0.1$. Dashed lines correspond to $\Lambda = 0.054 h^{-}$, $\bar\Lambda = 0.040 h^{-}$.
description: No data abstract available.
DOI: 10.17182/hepdata.99050.v1/t5
title: "TABLE I" of "Mid-rapidity Lambda and Antilambda production in Au + Au collisions at s(NN)**(1/2) = 130-GeV."

description: Fit parameters from Boltzmann and exponential fits of the $m_{T}$ spectra for $\Lambda$ and $\bar\Lambda$ at mid-rapidity ($|y|&lt;0.5$). Only statistical errors are presented. The systematic errors on $dN/dy$ and $T$ are approximately $10\%$. The Boltzmann form is adopted in Figure 2.
description: No data abstract available.
DOI: 10.17182/hepdata.99051.v1/t1
title: "Figure 1 (a)" of "Multiplicity fluctuations in Au + Au collisions at s(NN)**(1/2) = 130-GeV."

description: Dynamical fluctuations, $ν_{+−,dyn}$, measured in $|\eta| ≤ 0.5$ as a function of the collision centrality estimated with the total (uncorrected) multiplicity, M, in $|\eta| &lt; 0.75$. Only statistical errors are listed. Systematic errors estimated at $5\%$.
description: No data abstract available.
DOI: 10.17182/hepdata.99051.v1/t2
title: "Figure 1 (b)" of "Multiplicity fluctuations in Au + Au collisions at s(NN)**(1/2) = 130-GeV."

description: $\langle N\rangle ν_{+−,dyn}$ measured in $|\eta| ≤ 0.5$ vs M (opened circles) compared to the charge conservation limit (dotted line), resonance gas expectation based on ref.[5](solid line); and HIJING calculation (solid squares). Only statistical errors are listed. Systematic errors estimated at $10\%$.
description: No data abstract available.
DOI: 10.17182/hepdata.99051.v1/t3
title: "Figure 2" of "Multiplicity fluctuations in Au + Au collisions at s(NN)**(1/2) = 130-GeV."

description: Fluctuations $ν_{+−,dyn}$ for the $6\%$ most central collisions as a function of the range of integrated pseudorapidities. The expected limit due to charge conservation is shown as a dotted line.
description: No data abstract available.
DOI: 10.17182/hepdata.99052.v1/t1
title: "Figure 1" of "rho0 production and possible modification in Au + Au and p + p collisions at s(NN)**(1/2) = 200-GeV."

description: The raw $\pi^{+} \pi^{-}$ invariant mass distributions after subtraction of the like-sign reference distribution for minimum bias p+p (top) and peripheral Au+Au (bottom) interactions.
description: No data abstract available.
DOI: 10.3535/axt-4qk-qdn
title: Peperomia Ruiz & Pav.

description: Digital Specimen for the physical specimen hosted at Botanic Garden and Botanical Museum Berlin.
DOI: 10.3535/cag-l28-3dy
title: Goniothalamus gabriacianus (Baill.) Ast

description: Digital Specimen for the physical specimen hosted at Botanic Garden and Botanical Museum Berlin.
DOI: 10.17182/hepdata.99052.v1/t2
title: "Figure 1 inserted plot" of "rho0 production and possible modification in Au + Au and p + p collisions at s(NN)**(1/2) = 200-GeV."

description: The raw $\pi^{+} \pi^{-}$ invariant mass (solid line) and the like-sign reference distributions (open circles) for peripheral Au+Au collisions.
description: No data abstract available.
DOI: 10.17182/hepdata.99052.v1/t3
title: "Figure 2" of "rho0 production and possible modification in Au + Au and p + p collisions at s(NN)**(1/2) = 200-GeV."

description: The $\rho^{0}$ mass as a function of $p_{T}$ for minimum bias $p$+$p$ (filled circles), high multiplicity $p$+$p$ (open triangles), and peripheral Au+Au (filled squares) collisions. The error bars indicate the systematic uncertainty. Statistical errors are negligible. The $\rho^{0}$ mass was obtained by fitting the data to the BW×PS functional form described in the text. The dashed lines represent the average of the $\rho^{0}$ mass measured in $e^{+} e^{−}$. The shaded areas indicate the ρ0 mass measured in $p$+$p$ collisions. The open triangles have been shifted downward on the abscissa by $50$ MeV/$c$ for clarity.
description: No data abstract available.