cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.142463.v2/t124
title: "PbPb_5TeV_ptSpec" of "Multiplicity dependence of charged-particle production in pp, p-Pb, Xe-Xe and Pb-Pb collisions at the LHC"

description: Charged-particle transverse momentum spectra integrated over charged-particle multipliciy for PbPb collisions at 5.02 TeV.
description: CERN-LHC. ALICE. Multiplicity ($N_{\mathrm{ch}}$) distributions and transverse momentum ($p_{\mathrm{T}}$) spectra of inclusive primary charged particles in the kinematic range of $|\eta| &lt; 0.8$ and $0.15\ \mathrm{GeV}/c &lt; p_{\mathrm{T}} &lt; 10\ \mathrm{GeV}/c$ are reported for pp, p-Pb, Xe-Xe and Pb-Pb collisions at centre-of-mass energies per nucleon pair ranging from $\sqrt{s_\mathrm{NN}} = 2.76\ \mathrm{TeV}$ up to $13\ \mathrm{TeV}$. The multiplicity distributions are also shown in their KNO-scaled form. The correlation between the transverse momentum of primary charged particles and the charged-particle multiplicity of the corresponding collision is reported in fine intervals. In addition, the mean $ \langle p_{\mathrm{T}} \rangle $ and standard deviation $ \sigma(p_{\mathrm{T}}) $ derived from these multiplicity dependent $p_\mathrm{T}$ spectra are shown as a function of $N_{\mathrm{ch}}$. The relative standard deviation $ \sigma(p_{\mathrm{T}}) / \langle p_{\mathrm{T}} \rangle $ of the spectra is reported as well. All observables are also presented as a function of the reltaive multiplicity $ N_{\mathrm{ch}}\ / \langle N_{\mathrm{ch}} \rangle $. Note that $ \langle N_{\mathrm{ch}} \rangle $ is calculated for the whole multiplicity range extending beyond the $N_{\mathrm{ch}}$ values reported for the multiplicity-differential observables. Also the transverse momentum spectra integrated over this full range of multiplicities are presented. The mean and standard deviation derived from these multiplicity-integrated $p_\mathrm{T}$ spectra are used to normalize the corresponding multiplicity-dependent values which are then reported as a function of $ N_{\mathrm{ch}}\ / \langle N_{\mathrm{ch}} \rangle $.
DOI: 10.17182/hepdata.142463.v2/t125
title: "PbPb_5TeV_multPtSpec_scaled" of "Multiplicity dependence of charged-particle production in pp, p-Pb, Xe-Xe and Pb-Pb collisions at the LHC"

description: Charged-particle transverse momentum spectra as a function of relative charged-particle multiplicity for PbPb collisions at 5.02 TeV.
description: CERN-LHC. ALICE. Multiplicity ($N_{\mathrm{ch}}$) distributions and transverse momentum ($p_{\mathrm{T}}$) spectra of inclusive primary charged particles in the kinematic range of $|\eta| &lt; 0.8$ and $0.15\ \mathrm{GeV}/c &lt; p_{\mathrm{T}} &lt; 10\ \mathrm{GeV}/c$ are reported for pp, p-Pb, Xe-Xe and Pb-Pb collisions at centre-of-mass energies per nucleon pair ranging from $\sqrt{s_\mathrm{NN}} = 2.76\ \mathrm{TeV}$ up to $13\ \mathrm{TeV}$. The multiplicity distributions are also shown in their KNO-scaled form. The correlation between the transverse momentum of primary charged particles and the charged-particle multiplicity of the corresponding collision is reported in fine intervals. In addition, the mean $ \langle p_{\mathrm{T}} \rangle $ and standard deviation $ \sigma(p_{\mathrm{T}}) $ derived from these multiplicity dependent $p_\mathrm{T}$ spectra are shown as a function of $N_{\mathrm{ch}}$. The relative standard deviation $ \sigma(p_{\mathrm{T}}) / \langle p_{\mathrm{T}} \rangle $ of the spectra is reported as well. All observables are also presented as a function of the reltaive multiplicity $ N_{\mathrm{ch}}\ / \langle N_{\mathrm{ch}} \rangle $. Note that $ \langle N_{\mathrm{ch}} \rangle $ is calculated for the whole multiplicity range extending beyond the $N_{\mathrm{ch}}$ values reported for the multiplicity-differential observables. Also the transverse momentum spectra integrated over this full range of multiplicities are presented. The mean and standard deviation derived from these multiplicity-integrated $p_\mathrm{T}$ spectra are used to normalize the corresponding multiplicity-dependent values which are then reported as a function of $ N_{\mathrm{ch}}\ / \langle N_{\mathrm{ch}} \rangle $.
DOI: 10.17182/hepdata.142463.v2/t126
title: "PbPb_5TeV_multMeanPt_scaled" of "Multiplicity dependence of charged-particle production in pp, p-Pb, Xe-Xe and Pb-Pb collisions at the LHC"

description: Charged-particle mean transverse momentum as a function of relative charged-particle multiplicity for PbPb collisions at 5.02 TeV.
description: CERN-LHC. ALICE. Multiplicity ($N_{\mathrm{ch}}$) distributions and transverse momentum ($p_{\mathrm{T}}$) spectra of inclusive primary charged particles in the kinematic range of $|\eta| &lt; 0.8$ and $0.15\ \mathrm{GeV}/c &lt; p_{\mathrm{T}} &lt; 10\ \mathrm{GeV}/c$ are reported for pp, p-Pb, Xe-Xe and Pb-Pb collisions at centre-of-mass energies per nucleon pair ranging from $\sqrt{s_\mathrm{NN}} = 2.76\ \mathrm{TeV}$ up to $13\ \mathrm{TeV}$. The multiplicity distributions are also shown in their KNO-scaled form. The correlation between the transverse momentum of primary charged particles and the charged-particle multiplicity of the corresponding collision is reported in fine intervals. In addition, the mean $ \langle p_{\mathrm{T}} \rangle $ and standard deviation $ \sigma(p_{\mathrm{T}}) $ derived from these multiplicity dependent $p_\mathrm{T}$ spectra are shown as a function of $N_{\mathrm{ch}}$. The relative standard deviation $ \sigma(p_{\mathrm{T}}) / \langle p_{\mathrm{T}} \rangle $ of the spectra is reported as well. All observables are also presented as a function of the reltaive multiplicity $ N_{\mathrm{ch}}\ / \langle N_{\mathrm{ch}} \rangle $. Note that $ \langle N_{\mathrm{ch}} \rangle $ is calculated for the whole multiplicity range extending beyond the $N_{\mathrm{ch}}$ values reported for the multiplicity-differential observables. Also the transverse momentum spectra integrated over this full range of multiplicities are presented. The mean and standard deviation derived from these multiplicity-integrated $p_\mathrm{T}$ spectra are used to normalize the corresponding multiplicity-dependent values which are then reported as a function of $ N_{\mathrm{ch}}\ / \langle N_{\mathrm{ch}} \rangle $.
DOI: 10.17182/hepdata.142463.v2/t127
title: "PbPb_5TeV_multStdDevPt_scaled" of "Multiplicity dependence of charged-particle production in pp, p-Pb, Xe-Xe and Pb-Pb collisions at the LHC"

description: Standard deviation of charged-particle transverse momentum spectra as a function of relative charged-particle multiplicity for PbPb collisions at 5.02 TeV.
description: CERN-LHC. ALICE. Multiplicity ($N_{\mathrm{ch}}$) distributions and transverse momentum ($p_{\mathrm{T}}$) spectra of inclusive primary charged particles in the kinematic range of $|\eta| &lt; 0.8$ and $0.15\ \mathrm{GeV}/c &lt; p_{\mathrm{T}} &lt; 10\ \mathrm{GeV}/c$ are reported for pp, p-Pb, Xe-Xe and Pb-Pb collisions at centre-of-mass energies per nucleon pair ranging from $\sqrt{s_\mathrm{NN}} = 2.76\ \mathrm{TeV}$ up to $13\ \mathrm{TeV}$. The multiplicity distributions are also shown in their KNO-scaled form. The correlation between the transverse momentum of primary charged particles and the charged-particle multiplicity of the corresponding collision is reported in fine intervals. In addition, the mean $ \langle p_{\mathrm{T}} \rangle $ and standard deviation $ \sigma(p_{\mathrm{T}}) $ derived from these multiplicity dependent $p_\mathrm{T}$ spectra are shown as a function of $N_{\mathrm{ch}}$. The relative standard deviation $ \sigma(p_{\mathrm{T}}) / \langle p_{\mathrm{T}} \rangle $ of the spectra is reported as well. All observables are also presented as a function of the reltaive multiplicity $ N_{\mathrm{ch}}\ / \langle N_{\mathrm{ch}} \rangle $. Note that $ \langle N_{\mathrm{ch}} \rangle $ is calculated for the whole multiplicity range extending beyond the $N_{\mathrm{ch}}$ values reported for the multiplicity-differential observables. Also the transverse momentum spectra integrated over this full range of multiplicities are presented. The mean and standard deviation derived from these multiplicity-integrated $p_\mathrm{T}$ spectra are used to normalize the corresponding multiplicity-dependent values which are then reported as a function of $ N_{\mathrm{ch}}\ / \langle N_{\mathrm{ch}} \rangle $.
DOI: 10.17182/hepdata.142463.v2/t128
title: "PbPb_5TeV_multRelStdDevPt_scaled" of "Multiplicity dependence of charged-particle production in pp, p-Pb, Xe-Xe and Pb-Pb collisions at the LHC"

description: Standard deviation over mean of charged-particle transverse momentum spectra as a function of relative charged-particle multiplicity for PbPb collisions at 5.02 TeV.
description: CERN-LHC. ALICE. Multiplicity ($N_{\mathrm{ch}}$) distributions and transverse momentum ($p_{\mathrm{T}}$) spectra of inclusive primary charged particles in the kinematic range of $|\eta| &lt; 0.8$ and $0.15\ \mathrm{GeV}/c &lt; p_{\mathrm{T}} &lt; 10\ \mathrm{GeV}/c$ are reported for pp, p-Pb, Xe-Xe and Pb-Pb collisions at centre-of-mass energies per nucleon pair ranging from $\sqrt{s_\mathrm{NN}} = 2.76\ \mathrm{TeV}$ up to $13\ \mathrm{TeV}$. The multiplicity distributions are also shown in their KNO-scaled form. The correlation between the transverse momentum of primary charged particles and the charged-particle multiplicity of the corresponding collision is reported in fine intervals. In addition, the mean $ \langle p_{\mathrm{T}} \rangle $ and standard deviation $ \sigma(p_{\mathrm{T}}) $ derived from these multiplicity dependent $p_\mathrm{T}$ spectra are shown as a function of $N_{\mathrm{ch}}$. The relative standard deviation $ \sigma(p_{\mathrm{T}}) / \langle p_{\mathrm{T}} \rangle $ of the spectra is reported as well. All observables are also presented as a function of the reltaive multiplicity $ N_{\mathrm{ch}}\ / \langle N_{\mathrm{ch}} \rangle $. Note that $ \langle N_{\mathrm{ch}} \rangle $ is calculated for the whole multiplicity range extending beyond the $N_{\mathrm{ch}}$ values reported for the multiplicity-differential observables. Also the transverse momentum spectra integrated over this full range of multiplicities are presented. The mean and standard deviation derived from these multiplicity-integrated $p_\mathrm{T}$ spectra are used to normalize the corresponding multiplicity-dependent values which are then reported as a function of $ N_{\mathrm{ch}}\ / \langle N_{\mathrm{ch}} \rangle $.
DOI: 10.17182/hepdata.142463.v2/t129
title: "PbPb_5TeV_multMeanPtOverIncl_scaled" of "Multiplicity dependence of charged-particle production in pp, p-Pb, Xe-Xe and Pb-Pb collisions at the LHC"

description: Charged-particle mean transverse momentum divided by its multiplicity-integrated value as a function of relative charged-particle multiplicity for PbPb collisions at 5.02 TeV.
description: CERN-LHC. ALICE. Multiplicity ($N_{\mathrm{ch}}$) distributions and transverse momentum ($p_{\mathrm{T}}$) spectra of inclusive primary charged particles in the kinematic range of $|\eta| &lt; 0.8$ and $0.15\ \mathrm{GeV}/c &lt; p_{\mathrm{T}} &lt; 10\ \mathrm{GeV}/c$ are reported for pp, p-Pb, Xe-Xe and Pb-Pb collisions at centre-of-mass energies per nucleon pair ranging from $\sqrt{s_\mathrm{NN}} = 2.76\ \mathrm{TeV}$ up to $13\ \mathrm{TeV}$. The multiplicity distributions are also shown in their KNO-scaled form. The correlation between the transverse momentum of primary charged particles and the charged-particle multiplicity of the corresponding collision is reported in fine intervals. In addition, the mean $ \langle p_{\mathrm{T}} \rangle $ and standard deviation $ \sigma(p_{\mathrm{T}}) $ derived from these multiplicity dependent $p_\mathrm{T}$ spectra are shown as a function of $N_{\mathrm{ch}}$. The relative standard deviation $ \sigma(p_{\mathrm{T}}) / \langle p_{\mathrm{T}} \rangle $ of the spectra is reported as well. All observables are also presented as a function of the reltaive multiplicity $ N_{\mathrm{ch}}\ / \langle N_{\mathrm{ch}} \rangle $. Note that $ \langle N_{\mathrm{ch}} \rangle $ is calculated for the whole multiplicity range extending beyond the $N_{\mathrm{ch}}$ values reported for the multiplicity-differential observables. Also the transverse momentum spectra integrated over this full range of multiplicities are presented. The mean and standard deviation derived from these multiplicity-integrated $p_\mathrm{T}$ spectra are used to normalize the corresponding multiplicity-dependent values which are then reported as a function of $ N_{\mathrm{ch}}\ / \langle N_{\mathrm{ch}} \rangle $.
DOI: 10.17182/hepdata.142463.v2/t130
title: "PbPb_5TeV_multStdDevPtOverIncl_scaled" of "Multiplicity dependence of charged-particle production in pp, p-Pb, Xe-Xe and Pb-Pb collisions at the LHC"

description: Standard deviation of charged-particle transverse momentum spectra divided by its multiplicity-integrated value as a function of relative charged-particle multiplicity for PbPb collisions at 5.02 TeV.
description: CERN-LHC. ALICE. Multiplicity ($N_{\mathrm{ch}}$) distributions and transverse momentum ($p_{\mathrm{T}}$) spectra of inclusive primary charged particles in the kinematic range of $|\eta| &lt; 0.8$ and $0.15\ \mathrm{GeV}/c &lt; p_{\mathrm{T}} &lt; 10\ \mathrm{GeV}/c$ are reported for pp, p-Pb, Xe-Xe and Pb-Pb collisions at centre-of-mass energies per nucleon pair ranging from $\sqrt{s_\mathrm{NN}} = 2.76\ \mathrm{TeV}$ up to $13\ \mathrm{TeV}$. The multiplicity distributions are also shown in their KNO-scaled form. The correlation between the transverse momentum of primary charged particles and the charged-particle multiplicity of the corresponding collision is reported in fine intervals. In addition, the mean $ \langle p_{\mathrm{T}} \rangle $ and standard deviation $ \sigma(p_{\mathrm{T}}) $ derived from these multiplicity dependent $p_\mathrm{T}$ spectra are shown as a function of $N_{\mathrm{ch}}$. The relative standard deviation $ \sigma(p_{\mathrm{T}}) / \langle p_{\mathrm{T}} \rangle $ of the spectra is reported as well. All observables are also presented as a function of the reltaive multiplicity $ N_{\mathrm{ch}}\ / \langle N_{\mathrm{ch}} \rangle $. Note that $ \langle N_{\mathrm{ch}} \rangle $ is calculated for the whole multiplicity range extending beyond the $N_{\mathrm{ch}}$ values reported for the multiplicity-differential observables. Also the transverse momentum spectra integrated over this full range of multiplicities are presented. The mean and standard deviation derived from these multiplicity-integrated $p_\mathrm{T}$ spectra are used to normalize the corresponding multiplicity-dependent values which are then reported as a function of $ N_{\mathrm{ch}}\ / \langle N_{\mathrm{ch}} \rangle $.
DOI: 10.17182/hepdata.142604.v1/t1
title: "Figure 10" of "Nuclear-Modification Factor for Open-Heavy-Flavor Production at Forward Rapidity in Cu+Cu Collisions at sqrt(s_NN)=200 GeV"

description: Production cross section of negative muons from heavy-flavor mesons decay as a function of $p_T$ in $p$+$p$ collisions at $\sqrt{s}=200$ GeV.
description: Background: Heavy-flavor production in $p$+$p$ collisions tests perturbative-quantum-chromodynamics (pQCD) calculations. Modification of heavy-flavor production in heavy-ion collisions relative to binary-collision scaling from $p$+$p$ results, quantified with the nuclear-modification factor ($R_{AA}$), provides information on both cold- and hot-nuclear-matter effects. Midrapidity heavy-flavor $R_{AA}$ measurements at the Relativistic Heavy Ion Collider have challenged parton-energy-loss models and resulted in upper limits on the viscosity-entropy ratio that are near the quantum lower bound. Such measurements have not been made in the forward-rapidity region. Purpose: Determine transverse-momentum, $p_T$, spectra and the corresponding $R_{AA}$ for muons from heavy-flavor mesons decay in $p$+$p$ and Cu+Cu collisions at $\sqrt{s_{NN}}$=200 GeV and $y$=1.65. Method: Results are obtained using the semi-leptonic decay of heavy-flavor mesons into negative muons. The PHENIX muon-arm spectrometers measure the $p_T$ spectra of inclusive muon candidates. Backgrounds, primarily due to light hadrons, are determined with a Monte-Carlo calculation using a set of input hadron distributions tuned to match measured-hadron distributions in the same detector and statistically subtracted. Results: The charm-production cross section in $p$+$p$ collisions at $\sqrt{s}=200$ GeV, integrated over $p_T$ and in the rapidity range $1.4
DOI: 10.17182/hepdata.142604.v1/t2
title: "Figure 11a" of "Nuclear-Modification Factor for Open-Heavy-Flavor Production at Forward Rapidity in Cu+Cu Collisions at sqrt(s_NN)=200 GeV"

description: Invariant production yields of negative muons from heavy-flavor-mesons decay as a function $p_T$ in Cu+Cu collisions for three different centrality intervals (40-94%, 20-40%, and 0-20%), scaled by powers of ten for clarity. The solid line associated to each set of points corresponds to a fit to the $p$+$p$ invariant yield distribution described in the text, scaled by the appropriate number of binary collisions $N_{coll}$ when comparing to the Cu+Cu measurements.
description: Background: Heavy-flavor production in $p$+$p$ collisions tests perturbative-quantum-chromodynamics (pQCD) calculations. Modification of heavy-flavor production in heavy-ion collisions relative to binary-collision scaling from $p$+$p$ results, quantified with the nuclear-modification factor ($R_{AA}$), provides information on both cold- and hot-nuclear-matter effects. Midrapidity heavy-flavor $R_{AA}$ measurements at the Relativistic Heavy Ion Collider have challenged parton-energy-loss models and resulted in upper limits on the viscosity-entropy ratio that are near the quantum lower bound. Such measurements have not been made in the forward-rapidity region. Purpose: Determine transverse-momentum, $p_T$, spectra and the corresponding $R_{AA}$ for muons from heavy-flavor mesons decay in $p$+$p$ and Cu+Cu collisions at $\sqrt{s_{NN}}$=200 GeV and $y$=1.65. Method: Results are obtained using the semi-leptonic decay of heavy-flavor mesons into negative muons. The PHENIX muon-arm spectrometers measure the $p_T$ spectra of inclusive muon candidates. Backgrounds, primarily due to light hadrons, are determined with a Monte-Carlo calculation using a set of input hadron distributions tuned to match measured-hadron distributions in the same detector and statistically subtracted. Results: The charm-production cross section in $p$+$p$ collisions at $\sqrt{s}=200$ GeV, integrated over $p_T$ and in the rapidity range $1.4
DOI: 10.17182/hepdata.142604.v1/t3
title: "Figure 11b" of "Nuclear-Modification Factor for Open-Heavy-Flavor Production at Forward Rapidity in Cu+Cu Collisions at sqrt(s_NN)=200 GeV"

description: Invariant production yields of negative muons from heavy-flavor-mesons decay as a function $p_T$ in $p$+$p$ collisions at $\sqrt{s}=200$ GeV. The solid line associated to each set of points corresponds to a fit to the $p$+$p$ invariant yield distribution described in the text, scaled by the appropriate number of binary collisions $N_{coll}$ when comparing to the Cu+Cu measurements.
description: Background: Heavy-flavor production in $p$+$p$ collisions tests perturbative-quantum-chromodynamics (pQCD) calculations. Modification of heavy-flavor production in heavy-ion collisions relative to binary-collision scaling from $p$+$p$ results, quantified with the nuclear-modification factor ($R_{AA}$), provides information on both cold- and hot-nuclear-matter effects. Midrapidity heavy-flavor $R_{AA}$ measurements at the Relativistic Heavy Ion Collider have challenged parton-energy-loss models and resulted in upper limits on the viscosity-entropy ratio that are near the quantum lower bound. Such measurements have not been made in the forward-rapidity region. Purpose: Determine transverse-momentum, $p_T$, spectra and the corresponding $R_{AA}$ for muons from heavy-flavor mesons decay in $p$+$p$ and Cu+Cu collisions at $\sqrt{s_{NN}}$=200 GeV and $y$=1.65. Method: Results are obtained using the semi-leptonic decay of heavy-flavor mesons into negative muons. The PHENIX muon-arm spectrometers measure the $p_T$ spectra of inclusive muon candidates. Backgrounds, primarily due to light hadrons, are determined with a Monte-Carlo calculation using a set of input hadron distributions tuned to match measured-hadron distributions in the same detector and statistically subtracted. Results: The charm-production cross section in $p$+$p$ collisions at $\sqrt{s}=200$ GeV, integrated over $p_T$ and in the rapidity range $1.4
DOI: 10.17182/hepdata.142604.v1/t4
title: "Figure 12" of "Nuclear-Modification Factor for Open-Heavy-Flavor Production at Forward Rapidity in Cu+Cu Collisions at sqrt(s_NN)=200 GeV"

description: c$\bar{c}$ production cross section as a function of rapidity in $p$+$p$ collisions, measured using semileptonic decay to electrons (closed square) and to muons (closed circle).
description: Background: Heavy-flavor production in $p$+$p$ collisions tests perturbative-quantum-chromodynamics (pQCD) calculations. Modification of heavy-flavor production in heavy-ion collisions relative to binary-collision scaling from $p$+$p$ results, quantified with the nuclear-modification factor ($R_{AA}$), provides information on both cold- and hot-nuclear-matter effects. Midrapidity heavy-flavor $R_{AA}$ measurements at the Relativistic Heavy Ion Collider have challenged parton-energy-loss models and resulted in upper limits on the viscosity-entropy ratio that are near the quantum lower bound. Such measurements have not been made in the forward-rapidity region. Purpose: Determine transverse-momentum, $p_T$, spectra and the corresponding $R_{AA}$ for muons from heavy-flavor mesons decay in $p$+$p$ and Cu+Cu collisions at $\sqrt{s_{NN}}$=200 GeV and $y$=1.65. Method: Results are obtained using the semi-leptonic decay of heavy-flavor mesons into negative muons. The PHENIX muon-arm spectrometers measure the $p_T$ spectra of inclusive muon candidates. Backgrounds, primarily due to light hadrons, are determined with a Monte-Carlo calculation using a set of input hadron distributions tuned to match measured-hadron distributions in the same detector and statistically subtracted. Results: The charm-production cross section in $p$+$p$ collisions at $\sqrt{s}=200$ GeV, integrated over $p_T$ and in the rapidity range $1.4