cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.134676.v1/t8
title: "Table 8" of "Two-particle Bose-Einstein correlations and their Lévy parameters in PbPb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV"

description: The Levy scale parameter $R$ versus $\langle N_{\text{part}}\rangle^{1/3}$ in different $m_{\mathrm{T}}$ classes for negatively and positively charged hadron pairs. The bin range on $\langle N_{\text{part}}\rangle^{1/3}$ represents the 68% confidence interval associated to its uncertainty.
description: Two-particle Bose-Einstein momentum correlation functions for charged-hadron pairs in lead-lead collisions at a center-of-mass energy per nucleon pair of $\sqrt{s_{_{\mathrm{NN}}}} = 5.02$ TeV are studied. The data sample, containing $4.27\times 10^{9}$ events corresponding to an integrated luminosity of 0.607 $\mathrm{nb}^{-1}$, was collected by the CMS experiment in 2018. The experimental results are discussed in terms of a Levy-type source distribution. The parameters of this distribution are extracted as functions of particle pair average transverse mass and collision centrality. These parameters include the correlation strength parameter, the Levy index or shape parameter ($\alpha$), and the Levy scale parameter ($R$). The source shape, characterized by $\alpha$, is found to be neither Cauchy nor Gaussian, implying the need for a full Levy analysis. Similarly to what was previously found for systems characterized by Gaussian source radii, a hydrodynamical scaling is also observed for the Levy $R$ parameter.
DOI: 10.17182/hepdata.134676.v1/t9
title: "Table 9" of "Two-particle Bose-Einstein correlations and their Lévy parameters in PbPb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV"

description: The Levy stability index $\alpha$ versus the transverse mass $m_{\mathrm{T}}$ in different centrality classes for negatively and positively charged hadron pairs.
description: Two-particle Bose-Einstein momentum correlation functions for charged-hadron pairs in lead-lead collisions at a center-of-mass energy per nucleon pair of $\sqrt{s_{_{\mathrm{NN}}}} = 5.02$ TeV are studied. The data sample, containing $4.27\times 10^{9}$ events corresponding to an integrated luminosity of 0.607 $\mathrm{nb}^{-1}$, was collected by the CMS experiment in 2018. The experimental results are discussed in terms of a Levy-type source distribution. The parameters of this distribution are extracted as functions of particle pair average transverse mass and collision centrality. These parameters include the correlation strength parameter, the Levy index or shape parameter ($\alpha$), and the Levy scale parameter ($R$). The source shape, characterized by $\alpha$, is found to be neither Cauchy nor Gaussian, implying the need for a full Levy analysis. Similarly to what was previously found for systems characterized by Gaussian source radii, a hydrodynamical scaling is also observed for the Levy $R$ parameter.
DOI: 10.17182/hepdata.134676.v1/t10
title: "Table 10" of "Two-particle Bose-Einstein correlations and their Lévy parameters in PbPb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV"

description: The average Levy stability index $\langle \alpha \rangle$ versus $\langle N_{\text{part}}\rangle$ for both positively and negatively charged hadron pairs. The bin range on $\langle N_{\text{part}}\rangle$ represents the 68% confidence interval associated to its uncertainty.
description: Two-particle Bose-Einstein momentum correlation functions for charged-hadron pairs in lead-lead collisions at a center-of-mass energy per nucleon pair of $\sqrt{s_{_{\mathrm{NN}}}} = 5.02$ TeV are studied. The data sample, containing $4.27\times 10^{9}$ events corresponding to an integrated luminosity of 0.607 $\mathrm{nb}^{-1}$, was collected by the CMS experiment in 2018. The experimental results are discussed in terms of a Levy-type source distribution. The parameters of this distribution are extracted as functions of particle pair average transverse mass and collision centrality. These parameters include the correlation strength parameter, the Levy index or shape parameter ($\alpha$), and the Levy scale parameter ($R$). The source shape, characterized by $\alpha$, is found to be neither Cauchy nor Gaussian, implying the need for a full Levy analysis. Similarly to what was previously found for systems characterized by Gaussian source radii, a hydrodynamical scaling is also observed for the Levy $R$ parameter.
DOI: 10.17182/hepdata.134676.v1/t12
title: "Table 12" of "Two-particle Bose-Einstein correlations and their Lévy parameters in PbPb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV"

description: The correlation strength (re-scaled with the square of the pion fraction) $\lambda ^*$ versus the transverse mass $m_{\mathrm{T}}$ in different centrality classes for positively and negatively charged hadron pairs.
description: Two-particle Bose-Einstein momentum correlation functions for charged-hadron pairs in lead-lead collisions at a center-of-mass energy per nucleon pair of $\sqrt{s_{_{\mathrm{NN}}}} = 5.02$ TeV are studied. The data sample, containing $4.27\times 10^{9}$ events corresponding to an integrated luminosity of 0.607 $\mathrm{nb}^{-1}$, was collected by the CMS experiment in 2018. The experimental results are discussed in terms of a Levy-type source distribution. The parameters of this distribution are extracted as functions of particle pair average transverse mass and collision centrality. These parameters include the correlation strength parameter, the Levy index or shape parameter ($\alpha$), and the Levy scale parameter ($R$). The source shape, characterized by $\alpha$, is found to be neither Cauchy nor Gaussian, implying the need for a full Levy analysis. Similarly to what was previously found for systems characterized by Gaussian source radii, a hydrodynamical scaling is also observed for the Levy $R$ parameter.
DOI: 10.17182/hepdata.138867.v1/t1
title: "Table 1" of "Probing small Bjorken-$x$ nuclear gluonic structure via coherent J/$\psi$ photoproduction in ultraperipheral PbPb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV"

description: The differential coherent $\mathrm{J}/\psi$ photoproduction cross section as a function of rapidity, in different neutron multiplicity classes: 0n0n, 0nXn, XnXn , and AnAn.
description: No data abstract available.
DOI: 10.17182/hepdata.138867.v1/t2
title: "Table 2" of "Probing small Bjorken-$x$ nuclear gluonic structure via coherent J/$\psi$ photoproduction in ultraperipheral PbPb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV"

description: The total coherent $\mathrm{J}/\psi$ photoproduction cross section as a function of photon-nuclear center-of-mass energy per nucleon $W_{\gamma \mathrm{N}}^{\mathrm{Pb}}$, measured in PbPb ultra-peripheral collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV. The $W_{\gamma \mathrm{N}}^{\mathrm{Pb}}$ values used correspond to the center of each rapidity range. The theoretical uncertainties is due to the uncertainties in the photon flux.
description: No data abstract available.
DOI: 10.17182/hepdata.138867.v1/t3
title: "Table 3" of "Probing small Bjorken-$x$ nuclear gluonic structure via coherent J/$\psi$ photoproduction in ultraperipheral PbPb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV"

description: The nuclear gluon suppression factor $R_{\mathrm{g}}^{\mathrm{Pb}}$ as a function of Bjorken $x$ extracted from the CMS measurement of the coherent $\mathrm{J}/\psi$ photoproduction in PbPb ultra-peripheral collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV. The $x$ values are evaluated at the centers of their corresponding rapidity ranges. The theoretical uncertainties are due to the uncertainties in the photon flux and the impulse approximation model.
description: No data abstract available.
DOI: 10.17182/hepdata.138867.v1/t4
title: "Total covariance matrix" of "Probing small Bjorken-$x$ nuclear gluonic structure via coherent J/$\psi$ photoproduction in ultraperipheral PbPb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV"

description: The total covariance matrix of the total coherent photoproduction cross section as a function of photon-nuclear center-of-mass energy per nucleon $W_{\gamma \mathrm{N}}^{\mathrm{Pb}}$. The covariance matrix includes both the experimental and theoretical (photon flux) uncertainties. The bins are ordered as increasing in $W_{\gamma \mathrm{N}}^{\mathrm{Pb}}$.
description: No data abstract available.
DOI: 10.17182/hepdata.130960.v1/t1
title: "Figure 1a" of "Search for medium effects using jets from bottom quarks in PbPb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV"

description: Jet shapes, $\rho(\Delta r)$, for inclusive and b jets as function of $\Delta r$ from pp and PbPb collisions at $\sqrt{s_{NN}} = 5.02$ TeV.
description: The first study in heavy ion collisions of the shapes of jets arising from bottom (b) quarks is presented. Jet shapes are studied using charged hadron constituents as a function of their radial distance from the jet axis. Lead-lead (PbPb) collision data at a nucleon-nucleon center-of-mass energy of $\sqrt{s_{NN}}=5.02$~TeV were recorded by the CMS detector at the LHC, with an integrated luminosity of $1.69~\mathrm{nb}^{-1}$. Compared to proton-proton collisions, the quark-gluon plasma (QGP) created in PbPb collisions causes a redistribution of the energy in b jets to larger distances from the jet axis. This QGP-induced redistribution is substantially larger for b jets than for inclusive jets.
DOI: 10.17182/hepdata.130960.v1/t2
title: "Figure 1b" of "Search for medium effects using jets from bottom quarks in PbPb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV"

description: Jet shapes, $\rho(\Delta r)$, for inclusive and b jets as function of $\Delta r$ from pp and PbPb collisions at $\sqrt{s_{NN}} = 5.02$ TeV.
description: The first study in heavy ion collisions of the shapes of jets arising from bottom (b) quarks is presented. Jet shapes are studied using charged hadron constituents as a function of their radial distance from the jet axis. Lead-lead (PbPb) collision data at a nucleon-nucleon center-of-mass energy of $\sqrt{s_{NN}}=5.02$~TeV were recorded by the CMS detector at the LHC, with an integrated luminosity of $1.69~\mathrm{nb}^{-1}$. Compared to proton-proton collisions, the quark-gluon plasma (QGP) created in PbPb collisions causes a redistribution of the energy in b jets to larger distances from the jet axis. This QGP-induced redistribution is substantially larger for b jets than for inclusive jets.
DOI: 10.17182/hepdata.130960.v1/t3
title: "Figure 1c" of "Search for medium effects using jets from bottom quarks in PbPb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV"

description: Jet shapes, $\rho(\Delta r)$, for inclusive and b jets as function of $\Delta r$ from pp and PbPb collisions at $\sqrt{s_{NN}} = 5.02$ TeV.
description: The first study in heavy ion collisions of the shapes of jets arising from bottom (b) quarks is presented. Jet shapes are studied using charged hadron constituents as a function of their radial distance from the jet axis. Lead-lead (PbPb) collision data at a nucleon-nucleon center-of-mass energy of $\sqrt{s_{NN}}=5.02$~TeV were recorded by the CMS detector at the LHC, with an integrated luminosity of $1.69~\mathrm{nb}^{-1}$. Compared to proton-proton collisions, the quark-gluon plasma (QGP) created in PbPb collisions causes a redistribution of the energy in b jets to larger distances from the jet axis. This QGP-induced redistribution is substantially larger for b jets than for inclusive jets.
DOI: 10.17182/hepdata.130960.v1/t4
title: "Figure 1d" of "Search for medium effects using jets from bottom quarks in PbPb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV"

description: Jet shape ratios ($\rho(\Delta r)_{\mathrm{PbPb}}/\rho(\Delta r)_{\mathrm{pp}}$) for inclusive and b jets as function of $\Delta r$ at $\sqrt{s_{NN}} = 5.02$ TeV.
description: The first study in heavy ion collisions of the shapes of jets arising from bottom (b) quarks is presented. Jet shapes are studied using charged hadron constituents as a function of their radial distance from the jet axis. Lead-lead (PbPb) collision data at a nucleon-nucleon center-of-mass energy of $\sqrt{s_{NN}}=5.02$~TeV were recorded by the CMS detector at the LHC, with an integrated luminosity of $1.69~\mathrm{nb}^{-1}$. Compared to proton-proton collisions, the quark-gluon plasma (QGP) created in PbPb collisions causes a redistribution of the energy in b jets to larger distances from the jet axis. This QGP-induced redistribution is substantially larger for b jets than for inclusive jets.
DOI: 10.17182/hepdata.130960.v1/t5
title: "Figure 1e" of "Search for medium effects using jets from bottom quarks in PbPb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV"

description: Jet shape ratios ($\rho(\Delta r)_{\mathrm{PbPb}}/\rho(\Delta r)_{\mathrm{pp}}$) for inclusive and b jets as function of $\Delta r$ at $\sqrt{s_{NN}} = 5.02$ TeV.
description: The first study in heavy ion collisions of the shapes of jets arising from bottom (b) quarks is presented. Jet shapes are studied using charged hadron constituents as a function of their radial distance from the jet axis. Lead-lead (PbPb) collision data at a nucleon-nucleon center-of-mass energy of $\sqrt{s_{NN}}=5.02$~TeV were recorded by the CMS detector at the LHC, with an integrated luminosity of $1.69~\mathrm{nb}^{-1}$. Compared to proton-proton collisions, the quark-gluon plasma (QGP) created in PbPb collisions causes a redistribution of the energy in b jets to larger distances from the jet axis. This QGP-induced redistribution is substantially larger for b jets than for inclusive jets.
DOI: 10.17182/hepdata.138867.v1/t5
title: "Experimental covariance matrix" of "Probing small Bjorken-$x$ nuclear gluonic structure via coherent J/$\psi$ photoproduction in ultraperipheral PbPb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV"

description: The experimental covariance matrix of the total coherent photoproduction cross section as a function of photon-nuclear center-of-mass energy per nucleon $W_{\gamma \mathrm{N}}^{\mathrm{Pb}}$. The bins are ordered as increasing in $W_{\gamma \mathrm{N}}^{\mathrm{Pb}}$.
description: No data abstract available.
DOI: 10.17182/hepdata.138867.v1/t6
title: "Theoretical covariance matrix" of "Probing small Bjorken-$x$ nuclear gluonic structure via coherent J/$\psi$ photoproduction in ultraperipheral PbPb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV"

description: The theoretical (photon flux) covariance matrix of the total coherent photoproduction cross section as a function of photon-nuclear center-of-mass energy per nucleon $W_{\gamma \mathrm{N}}^{\mathrm{Pb}}$. The bins are ordered as increasing in $W_{\gamma \mathrm{N}}^{\mathrm{Pb}}$.
description: No data abstract available.
DOI: 10.17182/hepdata.130960.v1/t10
title: "Figure 1j" of "Search for medium effects using jets from bottom quarks in PbPb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV"

description: Jet shape ratios ($\rho(\Delta r)_{\mathrm{b}}/\rho(\Delta r)_{\mathrm{incl.}}$) as function of $\Delta r$ from pp and PbPb collisions at $\sqrt{s_{NN}}= 5.02$ TeV.
description: The first study in heavy ion collisions of the shapes of jets arising from bottom (b) quarks is presented. Jet shapes are studied using charged hadron constituents as a function of their radial distance from the jet axis. Lead-lead (PbPb) collision data at a nucleon-nucleon center-of-mass energy of $\sqrt{s_{NN}}=5.02$~TeV were recorded by the CMS detector at the LHC, with an integrated luminosity of $1.69~\mathrm{nb}^{-1}$. Compared to proton-proton collisions, the quark-gluon plasma (QGP) created in PbPb collisions causes a redistribution of the energy in b jets to larger distances from the jet axis. This QGP-induced redistribution is substantially larger for b jets than for inclusive jets.
DOI: 10.17182/hepdata.130960.v1/t11
title: "Figure 1k" of "Search for medium effects using jets from bottom quarks in PbPb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV"

description: Jet shape ratios ($\rho(\Delta r)_{\mathrm{b}}/\rho(\Delta r)_{\mathrm{incl.}}$) as function of $\Delta r$ from pp and PbPb collisions at $\sqrt{s_{NN}} = 5.02$ TeV.
description: The first study in heavy ion collisions of the shapes of jets arising from bottom (b) quarks is presented. Jet shapes are studied using charged hadron constituents as a function of their radial distance from the jet axis. Lead-lead (PbPb) collision data at a nucleon-nucleon center-of-mass energy of $\sqrt{s_{NN}}=5.02$~TeV were recorded by the CMS detector at the LHC, with an integrated luminosity of $1.69~\mathrm{nb}^{-1}$. Compared to proton-proton collisions, the quark-gluon plasma (QGP) created in PbPb collisions causes a redistribution of the energy in b jets to larger distances from the jet axis. This QGP-induced redistribution is substantially larger for b jets than for inclusive jets.
DOI: 10.17182/hepdata.130960.v1/t12
title: "Figure 1l" of "Search for medium effects using jets from bottom quarks in PbPb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV"

description: Jet shape ratios ($\rho(\Delta r)_{\mathrm{b}}/\rho(\Delta r)_{\mathrm{incl.}}$) as function of $\Delta r$ from pp and PbPb collisions at $\sqrt{s_{NN}} = 5.02$ TeV.
description: The first study in heavy ion collisions of the shapes of jets arising from bottom (b) quarks is presented. Jet shapes are studied using charged hadron constituents as a function of their radial distance from the jet axis. Lead-lead (PbPb) collision data at a nucleon-nucleon center-of-mass energy of $\sqrt{s_{NN}}=5.02$~TeV were recorded by the CMS detector at the LHC, with an integrated luminosity of $1.69~\mathrm{nb}^{-1}$. Compared to proton-proton collisions, the quark-gluon plasma (QGP) created in PbPb collisions causes a redistribution of the energy in b jets to larger distances from the jet axis. This QGP-induced redistribution is substantially larger for b jets than for inclusive jets.
DOI: 10.17182/hepdata.130960.v1/t6
title: "Figure 1f" of "Search for medium effects using jets from bottom quarks in PbPb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV"

description: Jet shape ratios ($\rho(\Delta r)_{\mathrm{PbPb}}/\rho(\Delta r)_{\mathrm{pp}}$) for inclusive and b jets as function of $\Delta r$ at $\sqrt{s_{NN}} = 5.02$ TeV.
description: The first study in heavy ion collisions of the shapes of jets arising from bottom (b) quarks is presented. Jet shapes are studied using charged hadron constituents as a function of their radial distance from the jet axis. Lead-lead (PbPb) collision data at a nucleon-nucleon center-of-mass energy of $\sqrt{s_{NN}}=5.02$~TeV were recorded by the CMS detector at the LHC, with an integrated luminosity of $1.69~\mathrm{nb}^{-1}$. Compared to proton-proton collisions, the quark-gluon plasma (QGP) created in PbPb collisions causes a redistribution of the energy in b jets to larger distances from the jet axis. This QGP-induced redistribution is substantially larger for b jets than for inclusive jets.
DOI: 10.17182/hepdata.130960.v1/t7
title: "Figure 1g" of "Search for medium effects using jets from bottom quarks in PbPb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV"

description: Transverse momentum profile difference $P(\Delta r)_{\mathrm{PbPb}}-P(\Delta r)_{\mathrm{pp}}$ vs. $\Delta r$ for inclusive and b jets at $\sqrt{s_{NN}} = 5.02$ TeV.
description: The first study in heavy ion collisions of the shapes of jets arising from bottom (b) quarks is presented. Jet shapes are studied using charged hadron constituents as a function of their radial distance from the jet axis. Lead-lead (PbPb) collision data at a nucleon-nucleon center-of-mass energy of $\sqrt{s_{NN}}=5.02$~TeV were recorded by the CMS detector at the LHC, with an integrated luminosity of $1.69~\mathrm{nb}^{-1}$. Compared to proton-proton collisions, the quark-gluon plasma (QGP) created in PbPb collisions causes a redistribution of the energy in b jets to larger distances from the jet axis. This QGP-induced redistribution is substantially larger for b jets than for inclusive jets.
DOI: 10.17182/hepdata.130960.v1/t8
title: "Figure 1h" of "Search for medium effects using jets from bottom quarks in PbPb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV"

description: Transverse momentum profile difference $P(\Delta r)_{\mathrm{PbPb}}-P(\Delta r)_{\mathrm{pp}}$ vs. $\Delta r$ for inclusive and b jets at $\sqrt{s_{NN}} = 5.02$ TeV.
description: The first study in heavy ion collisions of the shapes of jets arising from bottom (b) quarks is presented. Jet shapes are studied using charged hadron constituents as a function of their radial distance from the jet axis. Lead-lead (PbPb) collision data at a nucleon-nucleon center-of-mass energy of $\sqrt{s_{NN}}=5.02$~TeV were recorded by the CMS detector at the LHC, with an integrated luminosity of $1.69~\mathrm{nb}^{-1}$. Compared to proton-proton collisions, the quark-gluon plasma (QGP) created in PbPb collisions causes a redistribution of the energy in b jets to larger distances from the jet axis. This QGP-induced redistribution is substantially larger for b jets than for inclusive jets.
DOI: 10.17182/hepdata.130960.v1/t9
title: "Figure 1i" of "Search for medium effects using jets from bottom quarks in PbPb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV"

description: Transverse momentum profile difference $P(\Delta r)_{\mathrm{PbPb}}-P(\Delta r)_{\mathrm{pp}}$ vs. $\Delta r$ for inclusive and b jets at $\sqrt{s_{NN}} = 5.02$ TeV.
description: The first study in heavy ion collisions of the shapes of jets arising from bottom (b) quarks is presented. Jet shapes are studied using charged hadron constituents as a function of their radial distance from the jet axis. Lead-lead (PbPb) collision data at a nucleon-nucleon center-of-mass energy of $\sqrt{s_{NN}}=5.02$~TeV were recorded by the CMS detector at the LHC, with an integrated luminosity of $1.69~\mathrm{nb}^{-1}$. Compared to proton-proton collisions, the quark-gluon plasma (QGP) created in PbPb collisions causes a redistribution of the energy in b jets to larger distances from the jet axis. This QGP-induced redistribution is substantially larger for b jets than for inclusive jets.
DOI: 10.17182/hepdata.159930.v1/t1
title: "Figure 2a" of "Imaging nuclear shape through anisotropic and radial flow in high-energy heavy-ion collisions"

description: Data from Figure 2, panel a, $p(N_{ch}^{rec})$
description: No data abstract available.
DOI: 10.17182/hepdata.159930.v1/t10
title: "Figure 22a" of "Imaging nuclear shape through anisotropic and radial flow in high-energy heavy-ion collisions"

description: Data from Figure 22, panel a, U+U/Au+Au
description: No data abstract available.
DOI: 10.17182/hepdata.159930.v1/t2
title: "Figure 2b" of "Imaging nuclear shape through anisotropic and radial flow in high-energy heavy-ion collisions"

description: Data from Figure 2, panel b, $p(N_{ch}^{rec})$
description: No data abstract available.
DOI: 10.17182/hepdata.159930.v1/t3
title: "Figure 3a_0" of "Imaging nuclear shape through anisotropic and radial flow in high-energy heavy-ion collisions"

description: Data from Figure 3, panel a, Au+Au
description: No data abstract available.
DOI: 10.17182/hepdata.159930.v1/t4
title: "Figure 3a_1" of "Imaging nuclear shape through anisotropic and radial flow in high-energy heavy-ion collisions"

description: Data from Figure 3, panel a, U+U
description: No data abstract available.
DOI: 10.17182/hepdata.159930.v1/t5
title: "Figure 3b_0" of "Imaging nuclear shape through anisotropic and radial flow in high-energy heavy-ion collisions"

description: Data from Figure 3, panel b, Au+Au
description: No data abstract available.
DOI: 10.17182/hepdata.159930.v1/t6
title: "Figure 3b_1" of "Imaging nuclear shape through anisotropic and radial flow in high-energy heavy-ion collisions"

description: Data from Figure 3, panel b, U+U
description: No data abstract available.
DOI: 10.17182/hepdata.159930.v1/t7
title: "Figure 6a" of "Imaging nuclear shape through anisotropic and radial flow in high-energy heavy-ion collisions"

description: Data from Figure 6, panel a, 0-0.5% Centrality, 0.2
description: No data abstract available.