cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.3535/wns-mqf-t8m
title: Asteraceae Dumort.

description: Digital Specimen for the physical specimen hosted at Botanic Garden and Botanical Museum Berlin.
DOI: 10.17182/hepdata.98931.v1/t5
title: "Figure 7" 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 the invariant mass of pairs of oppositely charged $e^{\pm}$ candidates after sequentially applying the selection criteria described in Sec. IV A to both $e^{\pm}$ candidates.
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/t6
title: "Figure 8" 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 the invariant mass of $Z/\gamma^{*} \to e^{+}e^{−}$ candidate events satisfying all selection criteria described in Sec. IVC. The $Z/\gamma^{*} \to e^{+}e^{−}$ MC distribution (dashed line) is shown for comparison. Note the larger bin widths relative to Fig. 7
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/t7
title: "Figure 9 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) $E^{e}_{T}$ distribution of $W^{+}$ (top) and $W^{−}$ (bottom) candidate events, background components, and $W \to e\nu$ MC signal for comparison. Note the factor of two difference in the vertical scales.
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/t8
title: "Figure 9 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) $E^{e}_{T}$ distribution of $W^{+}$ (top) and $W^{−}$ (bottom) candidate events, background components, and $W \to e\nu$ MC signal for comparison. Note the factor of two difference in the vertical scales.
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: 10.25549/vercoutere-ouc110610677
title: 2 nude women standing in front of a glass-paned door

description: Back view of two nude females (one white outlined in flesh color and the other orange with brown details) standing in a room with a black floor in front of glass-paned door. See description of 001 for OT notes.
DOI: 10.3535/3xm-kkq-0r9
title: Cordia L.

description: Digital Specimen for the physical specimen hosted at Botanic Garden and Botanical Museum Berlin.
DOI: 10.17182/hepdata.98931.v1/t10
title: "Figure 10 right" 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) Lepton pseudorapidity distribution of $W^{+}$ (left) and $W^{−}$ (right) candidate events, background components, and $W \to e\nu$ MC signal for comparison.
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/t11
title: "Figure 12" 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) W cross section ratio, $R_{W}$, for the two $e^{\pm}$ pseudorapidity bins. Theory calculations at NLO from the fewz program using the MSTW08 and CTEQ 6.6 PDF sets (with 90% confidence level error eigenvector uncertainties) are shown for comparison.
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/t9
title: "Figure 10 left" 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) Lepton pseudorapidity distribution of $W^{+}$ (left) and $W^{−}$ (right) candidate events, background components, and $W \to e\nu$ MC signal for comparison.
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.98961.v1/t1
title: "Figure 1 a" of "Forward $\ensuremath{\Lambda}$ Production and Nuclear Stopping Power in $d$ + Au Collisions at $\sqrt{s_{NN}}$ = 200 GeV"

description: (Color online) a) Invariant mass distribution of $\Lambda$ candidates on the deuteron side with estimated $K_{s}^{0}$ background distribution, b) and c) show the background subtracted $\Lambda$ and $\overline{\Lambda}$ invariant mass distributions. The widths of the peaks are due to the limited momentum resolution of the detectors, and are reproduced by simulations.
description: We report the measurement of Lamda and Anti-Lamda yields and inverse slope parameters in d + Au collisions at $\sqrt{s_{NN}}$ = 200 GeV at forward and backward rapidities (y = $\pm$2.75), using data from the STAR forward time projection chambers. The contributions of different processes to baryon transport and particle production are probed exploiting the inherent asymmetry of the d + Au system. Comparisons to model calculations show that the baryon transport on the deuteron side is consistent with multiple collisions of the deuteron nucleons with gold participants. On the gold side HIJING based models do not describe the measured particle yields while models with initial state nuclear effects and/or hadronic rescattering do. The Multi-Chain Model can provide a good description of the net baryon density in d + Au collisions at RHIC, and the derived parameters of the model agree with those from nuclear collisions at lower energies.
DOI: 10.17182/hepdata.98961.v1/t2
title: "Figure 1 b" of "Forward $\ensuremath{\Lambda}$ Production and Nuclear Stopping Power in $d$ + Au Collisions at $\sqrt{s_{NN}}$ = 200 GeV"

description: (Color online) a) Invariant mass distribution of $\Lambda$ candidates on the deuteron side with estimated $K_{s}^{0}$ background distribution, b) and c) show the background subtracted $\Lambda$ and $\overline{\Lambda}$ invariant mass distributions. The widths of the peaks are due to the limited momentum resolution of the detectors, and are reproduced by simulations.
description: We report the measurement of Lamda and Anti-Lamda yields and inverse slope parameters in d + Au collisions at $\sqrt{s_{NN}}$ = 200 GeV at forward and backward rapidities (y = $\pm$2.75), using data from the STAR forward time projection chambers. The contributions of different processes to baryon transport and particle production are probed exploiting the inherent asymmetry of the d + Au system. Comparisons to model calculations show that the baryon transport on the deuteron side is consistent with multiple collisions of the deuteron nucleons with gold participants. On the gold side HIJING based models do not describe the measured particle yields while models with initial state nuclear effects and/or hadronic rescattering do. The Multi-Chain Model can provide a good description of the net baryon density in d + Au collisions at RHIC, and the derived parameters of the model agree with those from nuclear collisions at lower energies.
DOI: 10.17182/hepdata.98961.v1/t3
title: "Figure 1 c" of "Forward $\ensuremath{\Lambda}$ Production and Nuclear Stopping Power in $d$ + Au Collisions at $\sqrt{s_{NN}}$ = 200 GeV"

description: (Color online) a) Invariant mass distribution of $\Lambda$ candidates on the deuteron side with estimated $K_{s}^{0}$ background distribution, b) and c) show the background subtracted $\Lambda$ and $\overline{\Lambda}$ invariant mass distributions. The widths of the peaks are due to the limited momentum resolution of the detectors, and are reproduced by simulations.
description: We report the measurement of Lamda and Anti-Lamda yields and inverse slope parameters in d + Au collisions at $\sqrt{s_{NN}}$ = 200 GeV at forward and backward rapidities (y = $\pm$2.75), using data from the STAR forward time projection chambers. The contributions of different processes to baryon transport and particle production are probed exploiting the inherent asymmetry of the d + Au system. Comparisons to model calculations show that the baryon transport on the deuteron side is consistent with multiple collisions of the deuteron nucleons with gold participants. On the gold side HIJING based models do not describe the measured particle yields while models with initial state nuclear effects and/or hadronic rescattering do. The Multi-Chain Model can provide a good description of the net baryon density in d + Au collisions at RHIC, and the derived parameters of the model agree with those from nuclear collisions at lower energies.
DOI: 10.17182/hepdata.98961.v1/t4
title: "Figure 2" of "Forward $\ensuremath{\Lambda}$ Production and Nuclear Stopping Power in $d$ + Au Collisions at $\sqrt{s_{NN}}$ = 200 GeV"

description: (Color online) $\Lambda$ and $\overline{\Lambda}$ spectra on the deuteron and on the gold side in $d$ + Au minimum bias collisions. The data points on the gold side are multiplied by 2 for better visibility. The statistical errors are smaller than the points marking the measurements. The curves show a fit with a Boltzmann function in transverse mass to the data points.
description: We report the measurement of Lamda and Anti-Lamda yields and inverse slope parameters in d + Au collisions at $\sqrt{s_{NN}}$ = 200 GeV at forward and backward rapidities (y = $\pm$2.75), using data from the STAR forward time projection chambers. The contributions of different processes to baryon transport and particle production are probed exploiting the inherent asymmetry of the d + Au system. Comparisons to model calculations show that the baryon transport on the deuteron side is consistent with multiple collisions of the deuteron nucleons with gold participants. On the gold side HIJING based models do not describe the measured particle yields while models with initial state nuclear effects and/or hadronic rescattering do. The Multi-Chain Model can provide a good description of the net baryon density in d + Au collisions at RHIC, and the derived parameters of the model agree with those from nuclear collisions at lower energies.
DOI: 10.3535/9ev-ybc-p0n
title: Asteraceae Dumort.

description: Digital Specimen for the physical specimen hosted at Botanic Garden and Botanical Museum Berlin.
DOI: 10.3535/jr6-1ll-vw2
title: Phyllagathis Blume

description: Digital Specimen for the physical specimen hosted at Botanic Garden and Botanical Museum Berlin.
DOI: 10.17182/hepdata.98961.v1/t5
title: "Figure 3 a" of "Forward $\ensuremath{\Lambda}$ Production and Nuclear Stopping Power in $d$ + Au Collisions at $\sqrt{s_{NN}}$ = 200 GeV"

description: (Color online) (a) Comparison of the measured $\overline{\Lambda}$ yield with model calculations. Statistical errors are shown as vertical error bars, the vertical caps show the quadratic sum of statistical and systematic er- rors including the overall normalization uncertainty. In both panels the target and projectile beam rapidities are indicated by arrows.
description: We report the measurement of Lamda and Anti-Lamda yields and inverse slope parameters in d + Au collisions at $\sqrt{s_{NN}}$ = 200 GeV at forward and backward rapidities (y = $\pm$2.75), using data from the STAR forward time projection chambers. The contributions of different processes to baryon transport and particle production are probed exploiting the inherent asymmetry of the d + Au system. Comparisons to model calculations show that the baryon transport on the deuteron side is consistent with multiple collisions of the deuteron nucleons with gold participants. On the gold side HIJING based models do not describe the measured particle yields while models with initial state nuclear effects and/or hadronic rescattering do. The Multi-Chain Model can provide a good description of the net baryon density in d + Au collisions at RHIC, and the derived parameters of the model agree with those from nuclear collisions at lower energies.
DOI: 10.17182/hepdata.98961.v1/t6
title: "Figure 3 b" of "Forward $\ensuremath{\Lambda}$ Production and Nuclear Stopping Power in $d$ + Au Collisions at $\sqrt{s_{NN}}$ = 200 GeV"

description: (Color online) (b) Comparison of the net $\Lambda$ yield with model calculations. Statistical errors are shown as vertical error bars, the vertical caps show the quadratic sum of statistical and systematic er- rors including the overall normalization uncertainty. In both panels the target and projectile beam rapidities are indicated by arrows.
description: We report the measurement of Lamda and Anti-Lamda yields and inverse slope parameters in d + Au collisions at $\sqrt{s_{NN}}$ = 200 GeV at forward and backward rapidities (y = $\pm$2.75), using data from the STAR forward time projection chambers. The contributions of different processes to baryon transport and particle production are probed exploiting the inherent asymmetry of the d + Au system. Comparisons to model calculations show that the baryon transport on the deuteron side is consistent with multiple collisions of the deuteron nucleons with gold participants. On the gold side HIJING based models do not describe the measured particle yields while models with initial state nuclear effects and/or hadronic rescattering do. The Multi-Chain Model can provide a good description of the net baryon density in d + Au collisions at RHIC, and the derived parameters of the model agree with those from nuclear collisions at lower energies.
DOI: 10.17182/hepdata.98961.v1/t7
title: "Figure 4 bottom left" of "Forward $\ensuremath{\Lambda}$ Production and Nuclear Stopping Power in $d$ + Au Collisions at $\sqrt{s_{NN}}$ = 200 GeV"

description: (Color online) Comparison of $\overline{\Lambda}$ and net $\Lambda$ yields to model calculations for all three centrality classes. Statistical errors are shown as vertical error bars, the vertical caps show the quadratic sum of statistical and systematic errors. Beam rapidity is indicated by arrows.
description: We report the measurement of Lamda and Anti-Lamda yields and inverse slope parameters in d + Au collisions at $\sqrt{s_{NN}}$ = 200 GeV at forward and backward rapidities (y = $\pm$2.75), using data from the STAR forward time projection chambers. The contributions of different processes to baryon transport and particle production are probed exploiting the inherent asymmetry of the d + Au system. Comparisons to model calculations show that the baryon transport on the deuteron side is consistent with multiple collisions of the deuteron nucleons with gold participants. On the gold side HIJING based models do not describe the measured particle yields while models with initial state nuclear effects and/or hadronic rescattering do. The Multi-Chain Model can provide a good description of the net baryon density in d + Au collisions at RHIC, and the derived parameters of the model agree with those from nuclear collisions at lower energies.
DOI: 10.17182/hepdata.98961.v1/t8
title: "Figure 4 bottom middle" of "Forward $\ensuremath{\Lambda}$ Production and Nuclear Stopping Power in $d$ + Au Collisions at $\sqrt{s_{NN}}$ = 200 GeV"

description: (Color online) Comparison of $\overline{\Lambda}$ and net $\Lambda$ yields to model calculations for all three centrality classes. Statistical errors are shown as vertical error bars, the vertical caps show the quadratic sum of statistical and systematic errors. Beam rapidity is indicated by arrows.
description: We report the measurement of Lamda and Anti-Lamda yields and inverse slope parameters in d + Au collisions at $\sqrt{s_{NN}}$ = 200 GeV at forward and backward rapidities (y = $\pm$2.75), using data from the STAR forward time projection chambers. The contributions of different processes to baryon transport and particle production are probed exploiting the inherent asymmetry of the d + Au system. Comparisons to model calculations show that the baryon transport on the deuteron side is consistent with multiple collisions of the deuteron nucleons with gold participants. On the gold side HIJING based models do not describe the measured particle yields while models with initial state nuclear effects and/or hadronic rescattering do. The Multi-Chain Model can provide a good description of the net baryon density in d + Au collisions at RHIC, and the derived parameters of the model agree with those from nuclear collisions at lower energies.