cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.57373.v1/t8
title: "Table 8" of "Cold Nuclear Matter Effects on J/Psi as Constrained by Deuteron-Gold Measurements at sqrt(s_NN) = 200 GeV"

description: J/PSI invariant (1/(2PI*PT))*D2(N)/DPT/DYRAP versus centrality at forward rapidity (1.2
description: New analysis of the p+p and d+Au data recorded in 2003 and 2005 at the PHENIX experiment, at center-of-mass energy of 200GeV. Plots of the J/PSI invariant (1/(2PI*PT))*D2(N)/DPT/DYRAP, mean transverse momentum and nuclear modification factor RdA versus transverse momentum, rapidity and centrality are presented. The study also (1/(2PI*PT))*D2(N)/DPT/DYRAPed values for the breakup cross section of cc_bar pairs in cold nuclear matter The statistical errors are the combination of statistical error and uncorrelated point-to-point systematic error (i.e. which can move the points independently of each other), quadratically summed. The systematic error is the point-to-point correlated systematic errors (which can move the points coherently, thus not necessarly by the same amount).Global systematic are mentionned in comments, if necessary. Erratum : corrected values of breakup cross sections of cc_bar pairs presented in the article : "Cold Nuclear Matter Effects on J/Psi as Constrained by Deuteron-Gold Measurements at sqrt(s_NN) = 200 GeV" (IRN of the original paper : 7541414). arXiv reference of the original paper : arXiv:0711.3917v1.
DOI: 10.17182/hepdata.57373.v1/t9
title: "Table 9" of "Cold Nuclear Matter Effects on J/Psi as Constrained by Deuteron-Gold Measurements at sqrt(s_NN) = 200 GeV"

description: Nuclear modification factor versus rapidity in D+AU collisions, over 3 bins of rapidity.
description: New analysis of the p+p and d+Au data recorded in 2003 and 2005 at the PHENIX experiment, at center-of-mass energy of 200GeV. Plots of the J/PSI invariant (1/(2PI*PT))*D2(N)/DPT/DYRAP, mean transverse momentum and nuclear modification factor RdA versus transverse momentum, rapidity and centrality are presented. The study also (1/(2PI*PT))*D2(N)/DPT/DYRAPed values for the breakup cross section of cc_bar pairs in cold nuclear matter The statistical errors are the combination of statistical error and uncorrelated point-to-point systematic error (i.e. which can move the points independently of each other), quadratically summed. The systematic error is the point-to-point correlated systematic errors (which can move the points coherently, thus not necessarly by the same amount).Global systematic are mentionned in comments, if necessary. Erratum : corrected values of breakup cross sections of cc_bar pairs presented in the article : "Cold Nuclear Matter Effects on J/Psi as Constrained by Deuteron-Gold Measurements at sqrt(s_NN) = 200 GeV" (IRN of the original paper : 7541414). arXiv reference of the original paper : arXiv:0711.3917v1.
DOI: 10.17182/hepdata.57373.v1/t12
title: "Table 12" of "Cold Nuclear Matter Effects on J/Psi as Constrained by Deuteron-Gold Measurements at sqrt(s_NN) = 200 GeV"

description: Nuclear modification factor versus PT at mid rapidity (-0.35
description: New analysis of the p+p and d+Au data recorded in 2003 and 2005 at the PHENIX experiment, at center-of-mass energy of 200GeV. Plots of the J/PSI invariant (1/(2PI*PT))*D2(N)/DPT/DYRAP, mean transverse momentum and nuclear modification factor RdA versus transverse momentum, rapidity and centrality are presented. The study also (1/(2PI*PT))*D2(N)/DPT/DYRAPed values for the breakup cross section of cc_bar pairs in cold nuclear matter The statistical errors are the combination of statistical error and uncorrelated point-to-point systematic error (i.e. which can move the points independently of each other), quadratically summed. The systematic error is the point-to-point correlated systematic errors (which can move the points coherently, thus not necessarly by the same amount).Global systematic are mentionned in comments, if necessary. Erratum : corrected values of breakup cross sections of cc_bar pairs presented in the article : "Cold Nuclear Matter Effects on J/Psi as Constrained by Deuteron-Gold Measurements at sqrt(s_NN) = 200 GeV" (IRN of the original paper : 7541414). arXiv reference of the original paper : arXiv:0711.3917v1.
DOI: 10.17182/hepdata.57373.v1/t13
title: "Table 13" of "Cold Nuclear Matter Effects on J/Psi as Constrained by Deuteron-Gold Measurements at sqrt(s_NN) = 200 GeV"

description: Nuclear modification factor versus PT at forward rapidity (1.2
description: New analysis of the p+p and d+Au data recorded in 2003 and 2005 at the PHENIX experiment, at center-of-mass energy of 200GeV. Plots of the J/PSI invariant (1/(2PI*PT))*D2(N)/DPT/DYRAP, mean transverse momentum and nuclear modification factor RdA versus transverse momentum, rapidity and centrality are presented. The study also (1/(2PI*PT))*D2(N)/DPT/DYRAPed values for the breakup cross section of cc_bar pairs in cold nuclear matter The statistical errors are the combination of statistical error and uncorrelated point-to-point systematic error (i.e. which can move the points independently of each other), quadratically summed. The systematic error is the point-to-point correlated systematic errors (which can move the points coherently, thus not necessarly by the same amount).Global systematic are mentionned in comments, if necessary. Erratum : corrected values of breakup cross sections of cc_bar pairs presented in the article : "Cold Nuclear Matter Effects on J/Psi as Constrained by Deuteron-Gold Measurements at sqrt(s_NN) = 200 GeV" (IRN of the original paper : 7541414). arXiv reference of the original paper : arXiv:0711.3917v1.
DOI: 10.17182/hepdata.57373.v1/t14
title: "Table 14" of "Cold Nuclear Matter Effects on J/Psi as Constrained by Deuteron-Gold Measurements at sqrt(s_NN) = 200 GeV"

description: Nuclear modification factor versus centrality at backward rapidity (-2.2
description: New analysis of the p+p and d+Au data recorded in 2003 and 2005 at the PHENIX experiment, at center-of-mass energy of 200GeV. Plots of the J/PSI invariant (1/(2PI*PT))*D2(N)/DPT/DYRAP, mean transverse momentum and nuclear modification factor RdA versus transverse momentum, rapidity and centrality are presented. The study also (1/(2PI*PT))*D2(N)/DPT/DYRAPed values for the breakup cross section of cc_bar pairs in cold nuclear matter The statistical errors are the combination of statistical error and uncorrelated point-to-point systematic error (i.e. which can move the points independently of each other), quadratically summed. The systematic error is the point-to-point correlated systematic errors (which can move the points coherently, thus not necessarly by the same amount).Global systematic are mentionned in comments, if necessary. Erratum : corrected values of breakup cross sections of cc_bar pairs presented in the article : "Cold Nuclear Matter Effects on J/Psi as Constrained by Deuteron-Gold Measurements at sqrt(s_NN) = 200 GeV" (IRN of the original paper : 7541414). arXiv reference of the original paper : arXiv:0711.3917v1.
DOI: 10.17182/hepdata.57373.v1/t15
title: "Table 15" of "Cold Nuclear Matter Effects on J/Psi as Constrained by Deuteron-Gold Measurements at sqrt(s_NN) = 200 GeV"

description: Nuclear modification factor versus centrality at mid rapidity (-0.35
description: New analysis of the p+p and d+Au data recorded in 2003 and 2005 at the PHENIX experiment, at center-of-mass energy of 200GeV. Plots of the J/PSI invariant (1/(2PI*PT))*D2(N)/DPT/DYRAP, mean transverse momentum and nuclear modification factor RdA versus transverse momentum, rapidity and centrality are presented. The study also (1/(2PI*PT))*D2(N)/DPT/DYRAPed values for the breakup cross section of cc_bar pairs in cold nuclear matter The statistical errors are the combination of statistical error and uncorrelated point-to-point systematic error (i.e. which can move the points independently of each other), quadratically summed. The systematic error is the point-to-point correlated systematic errors (which can move the points coherently, thus not necessarly by the same amount).Global systematic are mentionned in comments, if necessary. Erratum : corrected values of breakup cross sections of cc_bar pairs presented in the article : "Cold Nuclear Matter Effects on J/Psi as Constrained by Deuteron-Gold Measurements at sqrt(s_NN) = 200 GeV" (IRN of the original paper : 7541414). arXiv reference of the original paper : arXiv:0711.3917v1.
DOI: 10.17182/hepdata.57373.v1/t16
title: "Table 16" of "Cold Nuclear Matter Effects on J/Psi as Constrained by Deuteron-Gold Measurements at sqrt(s_NN) = 200 GeV"

description: Nuclear modification factor versus centrality at forward rapidity (1.2
description: New analysis of the p+p and d+Au data recorded in 2003 and 2005 at the PHENIX experiment, at center-of-mass energy of 200GeV. Plots of the J/PSI invariant (1/(2PI*PT))*D2(N)/DPT/DYRAP, mean transverse momentum and nuclear modification factor RdA versus transverse momentum, rapidity and centrality are presented. The study also (1/(2PI*PT))*D2(N)/DPT/DYRAPed values for the breakup cross section of cc_bar pairs in cold nuclear matter The statistical errors are the combination of statistical error and uncorrelated point-to-point systematic error (i.e. which can move the points independently of each other), quadratically summed. The systematic error is the point-to-point correlated systematic errors (which can move the points coherently, thus not necessarly by the same amount).Global systematic are mentionned in comments, if necessary. Erratum : corrected values of breakup cross sections of cc_bar pairs presented in the article : "Cold Nuclear Matter Effects on J/Psi as Constrained by Deuteron-Gold Measurements at sqrt(s_NN) = 200 GeV" (IRN of the original paper : 7541414). arXiv reference of the original paper : arXiv:0711.3917v1.
DOI: 10.17182/hepdata.57373.v1/t17
title: "Table 17" of "Cold Nuclear Matter Effects on J/Psi as Constrained by Deuteron-Gold Measurements at sqrt(s_NN) = 200 GeV"

description: Mean PT^2 versus rapidity, extracted from a fit to the data, for DEUT + Au reactions. The mean value of PT^2 is calculated from the data for PT &lt; 5 Gev/c.
description: New analysis of the p+p and d+Au data recorded in 2003 and 2005 at the PHENIX experiment, at center-of-mass energy of 200GeV. Plots of the J/PSI invariant (1/(2PI*PT))*D2(N)/DPT/DYRAP, mean transverse momentum and nuclear modification factor RdA versus transverse momentum, rapidity and centrality are presented. The study also (1/(2PI*PT))*D2(N)/DPT/DYRAPed values for the breakup cross section of cc_bar pairs in cold nuclear matter The statistical errors are the combination of statistical error and uncorrelated point-to-point systematic error (i.e. which can move the points independently of each other), quadratically summed. The systematic error is the point-to-point correlated systematic errors (which can move the points coherently, thus not necessarly by the same amount).Global systematic are mentionned in comments, if necessary. Erratum : corrected values of breakup cross sections of cc_bar pairs presented in the article : "Cold Nuclear Matter Effects on J/Psi as Constrained by Deuteron-Gold Measurements at sqrt(s_NN) = 200 GeV" (IRN of the original paper : 7541414). arXiv reference of the original paper : arXiv:0711.3917v1.
DOI: 10.17182/hepdata.57373.v1/t18
title: "Table 18" of "Cold Nuclear Matter Effects on J/Psi as Constrained by Deuteron-Gold Measurements at sqrt(s_NN) = 200 GeV"

description: Mean PT^2 versus rapidity, extracted from a fit to the data, for P + P reactions. The mean value of PT^2 is calculated from the data for PT &lt; 5 Gev/c.
description: New analysis of the p+p and d+Au data recorded in 2003 and 2005 at the PHENIX experiment, at center-of-mass energy of 200GeV. Plots of the J/PSI invariant (1/(2PI*PT))*D2(N)/DPT/DYRAP, mean transverse momentum and nuclear modification factor RdA versus transverse momentum, rapidity and centrality are presented. The study also (1/(2PI*PT))*D2(N)/DPT/DYRAPed values for the breakup cross section of cc_bar pairs in cold nuclear matter The statistical errors are the combination of statistical error and uncorrelated point-to-point systematic error (i.e. which can move the points independently of each other), quadratically summed. The systematic error is the point-to-point correlated systematic errors (which can move the points coherently, thus not necessarly by the same amount).Global systematic are mentionned in comments, if necessary. Erratum : corrected values of breakup cross sections of cc_bar pairs presented in the article : "Cold Nuclear Matter Effects on J/Psi as Constrained by Deuteron-Gold Measurements at sqrt(s_NN) = 200 GeV" (IRN of the original paper : 7541414). arXiv reference of the original paper : arXiv:0711.3917v1.
DOI: 10.17182/hepdata.57373.v1/t19
title: "Table 19" of "Cold Nuclear Matter Effects on J/Psi as Constrained by Deuteron-Gold Measurements at sqrt(s_NN) = 200 GeV"

description: Breakup cross section of c-c_bar pairs inside cold nuclear matter,integrated over the whole domain of rapidity.The breakup cross section is calculated with two models of shadowing for nuclear PDFs ; the EKS model and the NDSG model. The uncertainties given, containing statistical and systematical error, are corresponding to one standard deviation.
description: New analysis of the p+p and d+Au data recorded in 2003 and 2005 at the PHENIX experiment, at center-of-mass energy of 200GeV. Plots of the J/PSI invariant (1/(2PI*PT))*D2(N)/DPT/DYRAP, mean transverse momentum and nuclear modification factor RdA versus transverse momentum, rapidity and centrality are presented. The study also (1/(2PI*PT))*D2(N)/DPT/DYRAPed values for the breakup cross section of cc_bar pairs in cold nuclear matter The statistical errors are the combination of statistical error and uncorrelated point-to-point systematic error (i.e. which can move the points independently of each other), quadratically summed. The systematic error is the point-to-point correlated systematic errors (which can move the points coherently, thus not necessarly by the same amount).Global systematic are mentionned in comments, if necessary. Erratum : corrected values of breakup cross sections of cc_bar pairs presented in the article : "Cold Nuclear Matter Effects on J/Psi as Constrained by Deuteron-Gold Measurements at sqrt(s_NN) = 200 GeV" (IRN of the original paper : 7541414). arXiv reference of the original paper : arXiv:0711.3917v1.
DOI: 10.17182/hepdata.57373.v1/t20
title: "Table 20" of "Cold Nuclear Matter Effects on J/Psi as Constrained by Deuteron-Gold Measurements at sqrt(s_NN) = 200 GeV"

description: Breakup cross section of c-c_bar pairs inside cold nuclear matter for different ranges of rapidity.The breakup cross section is calculated with two models of shadowing for nuclear PDFs ; the EKS model and the NDSG model. The uncertainties given, containing statistical and systematical error, are corresponding to one standard deviation.
description: New analysis of the p+p and d+Au data recorded in 2003 and 2005 at the PHENIX experiment, at center-of-mass energy of 200GeV. Plots of the J/PSI invariant (1/(2PI*PT))*D2(N)/DPT/DYRAP, mean transverse momentum and nuclear modification factor RdA versus transverse momentum, rapidity and centrality are presented. The study also (1/(2PI*PT))*D2(N)/DPT/DYRAPed values for the breakup cross section of cc_bar pairs in cold nuclear matter The statistical errors are the combination of statistical error and uncorrelated point-to-point systematic error (i.e. which can move the points independently of each other), quadratically summed. The systematic error is the point-to-point correlated systematic errors (which can move the points coherently, thus not necessarly by the same amount).Global systematic are mentionned in comments, if necessary. Erratum : corrected values of breakup cross sections of cc_bar pairs presented in the article : "Cold Nuclear Matter Effects on J/Psi as Constrained by Deuteron-Gold Measurements at sqrt(s_NN) = 200 GeV" (IRN of the original paper : 7541414). arXiv reference of the original paper : arXiv:0711.3917v1.
DOI: 10.17182/hepdata.57373.v1/t21
title: "Table 21" of "Cold Nuclear Matter Effects on J/Psi as Constrained by Deuteron-Gold Measurements at sqrt(s_NN) = 200 GeV"

description: Breakup cross section of c-c_bar pairs inside cold nuclear matter, integrated over the whole domain of rapidity.The breakup cross section is calculated with two models of shadowing for nuclear PDFs ; the EKS model and the NDSG model. The uncertainties given, containing statistical and systematical error, are corresponding to one standard deviation.
description: New analysis of the p+p and d+Au data recorded in 2003 and 2005 at the PHENIX experiment, at center-of-mass energy of 200GeV. Plots of the J/PSI invariant (1/(2PI*PT))*D2(N)/DPT/DYRAP, mean transverse momentum and nuclear modification factor RdA versus transverse momentum, rapidity and centrality are presented. The study also (1/(2PI*PT))*D2(N)/DPT/DYRAPed values for the breakup cross section of cc_bar pairs in cold nuclear matter The statistical errors are the combination of statistical error and uncorrelated point-to-point systematic error (i.e. which can move the points independently of each other), quadratically summed. The systematic error is the point-to-point correlated systematic errors (which can move the points coherently, thus not necessarly by the same amount).Global systematic are mentionned in comments, if necessary. Erratum : corrected values of breakup cross sections of cc_bar pairs presented in the article : "Cold Nuclear Matter Effects on J/Psi as Constrained by Deuteron-Gold Measurements at sqrt(s_NN) = 200 GeV" (IRN of the original paper : 7541414). arXiv reference of the original paper : arXiv:0711.3917v1.
DOI: 10.17182/hepdata.57373.v1/t22
title: "Table 22" of "Cold Nuclear Matter Effects on J/Psi as Constrained by Deuteron-Gold Measurements at sqrt(s_NN) = 200 GeV"

description: Breakup cross section of c-c_bar pairs inside cold nuclear matter for different ranges of rapidity.The breakup cross section is calculated with two models of shadowing for nuclear PDFs ; the EKS model and the NDSG model. The uncertainties given, containing statistical and systematical error, are corresponding to one standard deviation.
description: New analysis of the p+p and d+Au data recorded in 2003 and 2005 at the PHENIX experiment, at center-of-mass energy of 200GeV. Plots of the J/PSI invariant (1/(2PI*PT))*D2(N)/DPT/DYRAP, mean transverse momentum and nuclear modification factor RdA versus transverse momentum, rapidity and centrality are presented. The study also (1/(2PI*PT))*D2(N)/DPT/DYRAPed values for the breakup cross section of cc_bar pairs in cold nuclear matter The statistical errors are the combination of statistical error and uncorrelated point-to-point systematic error (i.e. which can move the points independently of each other), quadratically summed. The systematic error is the point-to-point correlated systematic errors (which can move the points coherently, thus not necessarly by the same amount).Global systematic are mentionned in comments, if necessary. Erratum : corrected values of breakup cross sections of cc_bar pairs presented in the article : "Cold Nuclear Matter Effects on J/Psi as Constrained by Deuteron-Gold Measurements at sqrt(s_NN) = 200 GeV" (IRN of the original paper : 7541414). arXiv reference of the original paper : arXiv:0711.3917v1.
DOI: 10.17182/hepdata.57411.v1/t1
title: "Table 1" of "Bottomonium and Drell-Yan production in p-A collisions at 450 GeV"

description: Drell-Yann (for the mass region MMUMU&gt;6GeV/c**2) and bottomonium cross sections, and their ratio.
description: CERN-SPS. Bottomonium and Drell-Yan production in p-A collisions at 450GeV.
DOI: 10.17182/hepdata.57411.v1/t2
title: "Table 2" of "Bottomonium and Drell-Yan production in p-A collisions at 450 GeV"

description: Mean pT and Mean PT**2 for Drell-Yann (4.5
description: CERN-SPS. Bottomonium and Drell-Yan production in p-A collisions at 450GeV.
DOI: 10.17182/hepdata.57411.v1/t3
title: "Table 3" of "Bottomonium and Drell-Yan production in p-A collisions at 450 GeV"

description: ALPHA parameter.
description: CERN-SPS. Bottomonium and Drell-Yan production in p-A collisions at 450GeV.
DOI: 10.17182/hepdata.57412.v1/t1
title: "Table 1" of "J/psi and psi' production and their normal nuclear absorption in proton nucleus collisions at 400-GeV."

description: Production cross sections, per taregt nucleon for J/PSI and PSI(3685) and for Drell-Yann dimuon in the mass range of 2.9-4.5 GeV/c**, integrated in the phase space windows of the measurement.
description: CERN-SPS. J/PSI andPSI(3685) production and their normal nuclear absorption in proton-nucleus collisions at 400 GeV.
DOI: 10.5281/zenodo.17523549
title: High-frequency Doppler data and GNSS TEC data during the SSC of 10 May 2024 Storm
DOI: 10.17182/hepdata.57412.v1/t2
title: "Table 2" of "J/psi and psi' production and their normal nuclear absorption in proton nucleus collisions at 400-GeV."

description: Ratios of J/PSI, PSI(3685) and Drel Yann production cross sections, and for Drell-Yann dimuon in the mass range of 2.9-4.5 GeV/c**, integrated in the phase space windows of the measurement.
description: CERN-SPS. J/PSI andPSI(3685) production and their normal nuclear absorption in proton-nucleus collisions at 400 GeV.
DOI: 10.17182/hepdata.57412.v1/t3
title: "Table 3" of "J/psi and psi' production and their normal nuclear absorption in proton nucleus collisions at 400-GeV."

description: Absorption cross-section obtained with Glauber fits results only from this analysis.
description: CERN-SPS. J/PSI andPSI(3685) production and their normal nuclear absorption in proton-nucleus collisions at 400 GeV.
DOI: 10.17182/hepdata.57412.v1/t4
title: "Table 4" of "J/psi and psi' production and their normal nuclear absorption in proton nucleus collisions at 400-GeV."

description: Absorption cross-section obtained with Glauber fits results combined with previous analysis.
description: CERN-SPS. J/PSI andPSI(3685) production and their normal nuclear absorption in proton-nucleus collisions at 400 GeV.
DOI: 10.17182/hepdata.57420.v1/t1
title: "Table 1" of "psi' production in Pb-Pb collisions at 158 GeV/nucleon"

description: Inclusive cross sections for PSI(3685) and J/PSI, multiplied by their Branching ratios into MU+MU-,.
description: CERN-SPS. PSI(3685) production in Pb-Pb colisions at 158 GeV/nucleon Incertitude are R.M.S. from fit.RE = PB PB --&gt; J/PSI X.
DOI: 10.17182/hepdata.57420.v1/t2
title: "Table 2" of "psi' production in Pb-Pb collisions at 158 GeV/nucleon"

description: Inclusive cross sections for Drell Yan in the 4.2-7 GeV/c** mass range.
description: CERN-SPS. PSI(3685) production in Pb-Pb colisions at 158 GeV/nucleon Incertitude are R.M.S. from fit.RE = PB PB --&gt; J/PSI X.
DOI: 10.5281/zenodo.17523548
title: High-frequency Doppler data and GNSS TEC data during the SSC of 10 May 2024 Storm
DOI: 10.17182/hepdata.57420.v1/t3
title: "Table 3" of "psi' production in Pb-Pb collisions at 158 GeV/nucleon"

description: Inclusive cross sections for PSI(3685) and J/PSI, multiplied by theirBransching ratios into MU+MU-, and for Drell Yan in the 4.2-7 GeV/c** massrange.
description: CERN-SPS. PSI(3685) production in Pb-Pb colisions at 158 GeV/nucleon Incertitude are R.M.S. from fit.RE = PB PB --&gt; J/PSI X.
DOI: 10.3535/3n3-mxd-y6m
title: Plantae

description: Digital Specimen for the physical specimen hosted at Naturalis Biodiversity Center.
DOI: 10.3535/6jv-sry-2ag
title: Plantae

description: Digital Specimen for the physical specimen hosted at Naturalis Biodiversity Center.
DOI: 10.3535/7ej-zhk-267
title: Plantae

description: Digital Specimen for the physical specimen hosted at Naturalis Biodiversity Center.
DOI: 10.3535/6vd-lee-skb
title: Rusa C. H. Smith, 1827

description: Digital Specimen for the physical specimen hosted at Naturalis Biodiversity Center.
DOI: 10.3535/s1x-07y-gbx
title: Orthiopteris Copel.

description: Digital Specimen for the physical specimen hosted at Naturalis Biodiversity Center.
DOI: 10.3535/wrs-blp-02t
title: Plantae

description: Digital Specimen for the physical specimen hosted at Naturalis Biodiversity Center.