cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.168549.v1/t5
title: "Table 5" of "Medium-induced modification of azimuthal correlations of electrons from heavy-flavor hadron decays with charged particles in Pb-Pb collisions at $\sqrt{s_{\rm{NN}} = 5.02}$ TeV"

description: Baseline subtracted $\Delta\varphi$ correlation distribution between electrons from heavy-flavor hadron decays and associated charged particles for $4 &lt; p_\mathrm{T}^\mathrm{e} &lt; 12$ GeV/$c$ and $1 &lt; p_\mathrm{T}^\mathrm{assoc} &lt; 7$ GeV/c in Pb--Pb collisions in the 30--50% centrality class at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV.
description: The azimuthal-correlation distributions between electrons from the decays of heavy-flavor hadrons and associated charged particles in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV are reported for the 0--10\% and 30--50\% centrality classes. This measurement provides access to the jet-like correlation observables in the heavy-flavor sector in Pb--Pb collisions. The analysis is performed for trigger electrons from heavy-flavor hadron decays with transverse momentum $4 &lt; p_\mathrm{T}^\mathrm{e} &lt; 16~{\mathrm GeV}/c$, considering associated particles within the transverse-momentum range $1 &lt; p_\mathrm{T}^\mathrm{assoc} &lt; 7$ ${\mathrm GeV}/c$, and a pseudorapidity difference of $|\Delta\eta|&lt;1$ between the trigger electron and associated particles. The per-trigger nuclear modification factor ($I_\mathrm{AA}$) is calculated to compare the near- and away-side peak yields to those in pp collisions at $\sqrt{s} = 5.02$ TeV. In 0--10\% central collisions, the $I_\mathrm{AA}$ indicates a hint of enhancement of associated-particle yields with $p_\mathrm{T}&lt;3$ GeV/$c$ on the near side, and a suppression of yields with $p_\mathrm{T}&gt;4$ GeV/$c$ on the away side. The $I_\mathrm{AA}$ for electron triggers from heavy-flavor hadron decays is compared with that for light-flavor and strange-particle triggers to investigate the dependence on different fragmentation processes and parton-medium dynamics, and is found to be the same within uncertainties.
DOI: 10.17182/hepdata.168549.v1/t6
title: "Table 6" of "Medium-induced modification of azimuthal correlations of electrons from heavy-flavor hadron decays with charged particles in Pb-Pb collisions at $\sqrt{s_{\rm{NN}} = 5.02}$ TeV"

description: Baseline subtracted $\Delta\varphi$ correlation distribution between electrons from heavy-flavor hadron decays and associated charged particles for $4 &lt; p_\mathrm{T}^\mathrm{e} &lt; 12$ GeV/$c$ and $1 &lt; p_\mathrm{T}^\mathrm{assoc} &lt; 7$ GeV/c in pp collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV.
description: The azimuthal-correlation distributions between electrons from the decays of heavy-flavor hadrons and associated charged particles in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV are reported for the 0--10\% and 30--50\% centrality classes. This measurement provides access to the jet-like correlation observables in the heavy-flavor sector in Pb--Pb collisions. The analysis is performed for trigger electrons from heavy-flavor hadron decays with transverse momentum $4 &lt; p_\mathrm{T}^\mathrm{e} &lt; 16~{\mathrm GeV}/c$, considering associated particles within the transverse-momentum range $1 &lt; p_\mathrm{T}^\mathrm{assoc} &lt; 7$ ${\mathrm GeV}/c$, and a pseudorapidity difference of $|\Delta\eta|&lt;1$ between the trigger electron and associated particles. The per-trigger nuclear modification factor ($I_\mathrm{AA}$) is calculated to compare the near- and away-side peak yields to those in pp collisions at $\sqrt{s} = 5.02$ TeV. In 0--10\% central collisions, the $I_\mathrm{AA}$ indicates a hint of enhancement of associated-particle yields with $p_\mathrm{T}&lt;3$ GeV/$c$ on the near side, and a suppression of yields with $p_\mathrm{T}&gt;4$ GeV/$c$ on the away side. The $I_\mathrm{AA}$ for electron triggers from heavy-flavor hadron decays is compared with that for light-flavor and strange-particle triggers to investigate the dependence on different fragmentation processes and parton-medium dynamics, and is found to be the same within uncertainties.
DOI: 10.17182/hepdata.168549.v1/t7
title: "Table 7" of "Medium-induced modification of azimuthal correlations of electrons from heavy-flavor hadron decays with charged particles in Pb-Pb collisions at $\sqrt{s_{\rm{NN}} = 5.02}$ TeV"

description: Associated yield of near-side (NS) $\Delta\varphi$ correlation distribution between electrons from heavy-flavor hadron decays and associated charged particles as a function of $p_\mathrm{T}^\mathrm{assoc}$ for $4 &lt; p_\mathrm{T}^\mathrm{e} &lt; 12$ GeV/$c$ in Pb--Pb collisions in the 0--10% and 30--50% centrality classes compared to pp, at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV.
description: The azimuthal-correlation distributions between electrons from the decays of heavy-flavor hadrons and associated charged particles in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV are reported for the 0--10\% and 30--50\% centrality classes. This measurement provides access to the jet-like correlation observables in the heavy-flavor sector in Pb--Pb collisions. The analysis is performed for trigger electrons from heavy-flavor hadron decays with transverse momentum $4 &lt; p_\mathrm{T}^\mathrm{e} &lt; 16~{\mathrm GeV}/c$, considering associated particles within the transverse-momentum range $1 &lt; p_\mathrm{T}^\mathrm{assoc} &lt; 7$ ${\mathrm GeV}/c$, and a pseudorapidity difference of $|\Delta\eta|&lt;1$ between the trigger electron and associated particles. The per-trigger nuclear modification factor ($I_\mathrm{AA}$) is calculated to compare the near- and away-side peak yields to those in pp collisions at $\sqrt{s} = 5.02$ TeV. In 0--10\% central collisions, the $I_\mathrm{AA}$ indicates a hint of enhancement of associated-particle yields with $p_\mathrm{T}&lt;3$ GeV/$c$ on the near side, and a suppression of yields with $p_\mathrm{T}&gt;4$ GeV/$c$ on the away side. The $I_\mathrm{AA}$ for electron triggers from heavy-flavor hadron decays is compared with that for light-flavor and strange-particle triggers to investigate the dependence on different fragmentation processes and parton-medium dynamics, and is found to be the same within uncertainties.
DOI: 10.17182/hepdata.168549.v1/t8
title: "Table 8" of "Medium-induced modification of azimuthal correlations of electrons from heavy-flavor hadron decays with charged particles in Pb-Pb collisions at $\sqrt{s_{\rm{NN}} = 5.02}$ TeV"

description: Associated yield of away-side (AS) $\Delta\varphi$ correlation distribution between electrons from heavy-flavor hadron decays and associated charged particles as a function of $p_\mathrm{T}^\mathrm{assoc}$ for $4 &lt; p_\mathrm{T}^\mathrm{e} &lt; 12$ GeV/$c$ in Pb--Pb collisions in the 0--10% and 30--50% centrality classes compared to pp, at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV.
description: The azimuthal-correlation distributions between electrons from the decays of heavy-flavor hadrons and associated charged particles in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV are reported for the 0--10\% and 30--50\% centrality classes. This measurement provides access to the jet-like correlation observables in the heavy-flavor sector in Pb--Pb collisions. The analysis is performed for trigger electrons from heavy-flavor hadron decays with transverse momentum $4 &lt; p_\mathrm{T}^\mathrm{e} &lt; 16~{\mathrm GeV}/c$, considering associated particles within the transverse-momentum range $1 &lt; p_\mathrm{T}^\mathrm{assoc} &lt; 7$ ${\mathrm GeV}/c$, and a pseudorapidity difference of $|\Delta\eta|&lt;1$ between the trigger electron and associated particles. The per-trigger nuclear modification factor ($I_\mathrm{AA}$) is calculated to compare the near- and away-side peak yields to those in pp collisions at $\sqrt{s} = 5.02$ TeV. In 0--10\% central collisions, the $I_\mathrm{AA}$ indicates a hint of enhancement of associated-particle yields with $p_\mathrm{T}&lt;3$ GeV/$c$ on the near side, and a suppression of yields with $p_\mathrm{T}&gt;4$ GeV/$c$ on the away side. The $I_\mathrm{AA}$ for electron triggers from heavy-flavor hadron decays is compared with that for light-flavor and strange-particle triggers to investigate the dependence on different fragmentation processes and parton-medium dynamics, and is found to be the same within uncertainties.
DOI: 10.17182/hepdata.168549.v1/t9
title: "Table 9" of "Medium-induced modification of azimuthal correlations of electrons from heavy-flavor hadron decays with charged particles in Pb-Pb collisions at $\sqrt{s_{\rm{NN}} = 5.02}$ TeV"

description: Associated yield of near-side (NS) $\Delta\varphi$ correlation distribution between electrons from heavy-flavor hadron decays and associated charged particles as a function of $p_\mathrm{T}^\mathrm{assoc}$ for $4 &lt; p_\mathrm{T}^\mathrm{e} &lt; 7$ GeV/$c$ and $7 &lt; p_\mathrm{T}^\mathrm{e} &lt; 16$ GeV/$c$ in Pb--Pb collisions in the 0--10% centrality class and pp collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV.
description: The azimuthal-correlation distributions between electrons from the decays of heavy-flavor hadrons and associated charged particles in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV are reported for the 0--10\% and 30--50\% centrality classes. This measurement provides access to the jet-like correlation observables in the heavy-flavor sector in Pb--Pb collisions. The analysis is performed for trigger electrons from heavy-flavor hadron decays with transverse momentum $4 &lt; p_\mathrm{T}^\mathrm{e} &lt; 16~{\mathrm GeV}/c$, considering associated particles within the transverse-momentum range $1 &lt; p_\mathrm{T}^\mathrm{assoc} &lt; 7$ ${\mathrm GeV}/c$, and a pseudorapidity difference of $|\Delta\eta|&lt;1$ between the trigger electron and associated particles. The per-trigger nuclear modification factor ($I_\mathrm{AA}$) is calculated to compare the near- and away-side peak yields to those in pp collisions at $\sqrt{s} = 5.02$ TeV. In 0--10\% central collisions, the $I_\mathrm{AA}$ indicates a hint of enhancement of associated-particle yields with $p_\mathrm{T}&lt;3$ GeV/$c$ on the near side, and a suppression of yields with $p_\mathrm{T}&gt;4$ GeV/$c$ on the away side. The $I_\mathrm{AA}$ for electron triggers from heavy-flavor hadron decays is compared with that for light-flavor and strange-particle triggers to investigate the dependence on different fragmentation processes and parton-medium dynamics, and is found to be the same within uncertainties.
DOI: 10.17182/hepdata.168549.v1/t10
title: "Table 10" of "Medium-induced modification of azimuthal correlations of electrons from heavy-flavor hadron decays with charged particles in Pb-Pb collisions at $\sqrt{s_{\rm{NN}} = 5.02}$ TeV"

description: Associated yield of away-side (AS) $\Delta\varphi$ correlation distribution between electrons from heavy-flavor hadron decays and associated charged particles as a function of $p_\mathrm{T}^\mathrm{assoc}$ for $4 &lt; p_\mathrm{T}^\mathrm{e} &lt; 7$ GeV/$c$ and $7 &lt; p_\mathrm{T}^\mathrm{e} &lt; 16$ GeV/$c$ in Pb--Pb collisions in the 0--10% centrality class and pp collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV.
description: The azimuthal-correlation distributions between electrons from the decays of heavy-flavor hadrons and associated charged particles in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV are reported for the 0--10\% and 30--50\% centrality classes. This measurement provides access to the jet-like correlation observables in the heavy-flavor sector in Pb--Pb collisions. The analysis is performed for trigger electrons from heavy-flavor hadron decays with transverse momentum $4 &lt; p_\mathrm{T}^\mathrm{e} &lt; 16~{\mathrm GeV}/c$, considering associated particles within the transverse-momentum range $1 &lt; p_\mathrm{T}^\mathrm{assoc} &lt; 7$ ${\mathrm GeV}/c$, and a pseudorapidity difference of $|\Delta\eta|&lt;1$ between the trigger electron and associated particles. The per-trigger nuclear modification factor ($I_\mathrm{AA}$) is calculated to compare the near- and away-side peak yields to those in pp collisions at $\sqrt{s} = 5.02$ TeV. In 0--10\% central collisions, the $I_\mathrm{AA}$ indicates a hint of enhancement of associated-particle yields with $p_\mathrm{T}&lt;3$ GeV/$c$ on the near side, and a suppression of yields with $p_\mathrm{T}&gt;4$ GeV/$c$ on the away side. The $I_\mathrm{AA}$ for electron triggers from heavy-flavor hadron decays is compared with that for light-flavor and strange-particle triggers to investigate the dependence on different fragmentation processes and parton-medium dynamics, and is found to be the same within uncertainties.
DOI: 10.17182/hepdata.168549.v1/t12
title: "Table 12" of "Medium-induced modification of azimuthal correlations of electrons from heavy-flavor hadron decays with charged particles in Pb-Pb collisions at $\sqrt{s_{\rm{NN}} = 5.02}$ TeV"

description: Per-trigger nuclear modification factor ($I_\mathrm{AA}$) of away-side (AS) $\Delta\varphi$ correlation distribution between electrons from heavy-flavor hadron decays and associated charged particles as a function of $p_\mathrm{T}^\mathrm{assoc}$ for $4 &lt; p_\mathrm{T}^\mathrm{e} &lt; 12$ GeV/$c$ in Pb--Pb collisions in the 0--10% and 30--50% centrality classes compared to pp, at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV.
description: The azimuthal-correlation distributions between electrons from the decays of heavy-flavor hadrons and associated charged particles in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV are reported for the 0--10\% and 30--50\% centrality classes. This measurement provides access to the jet-like correlation observables in the heavy-flavor sector in Pb--Pb collisions. The analysis is performed for trigger electrons from heavy-flavor hadron decays with transverse momentum $4 &lt; p_\mathrm{T}^\mathrm{e} &lt; 16~{\mathrm GeV}/c$, considering associated particles within the transverse-momentum range $1 &lt; p_\mathrm{T}^\mathrm{assoc} &lt; 7$ ${\mathrm GeV}/c$, and a pseudorapidity difference of $|\Delta\eta|&lt;1$ between the trigger electron and associated particles. The per-trigger nuclear modification factor ($I_\mathrm{AA}$) is calculated to compare the near- and away-side peak yields to those in pp collisions at $\sqrt{s} = 5.02$ TeV. In 0--10\% central collisions, the $I_\mathrm{AA}$ indicates a hint of enhancement of associated-particle yields with $p_\mathrm{T}&lt;3$ GeV/$c$ on the near side, and a suppression of yields with $p_\mathrm{T}&gt;4$ GeV/$c$ on the away side. The $I_\mathrm{AA}$ for electron triggers from heavy-flavor hadron decays is compared with that for light-flavor and strange-particle triggers to investigate the dependence on different fragmentation processes and parton-medium dynamics, and is found to be the same within uncertainties.
DOI: 10.17182/hepdata.168549.v1/t13
title: "Table 13" of "Medium-induced modification of azimuthal correlations of electrons from heavy-flavor hadron decays with charged particles in Pb-Pb collisions at $\sqrt{s_{\rm{NN}} = 5.02}$ TeV"

description: Per-trigger nuclear modification factor ($I_\mathrm{AA}$) of near-side (NS) $\Delta\varphi$ correlation distribution between electrons from heavy-flavor hadron decays and associated charged particles as a function of $p_\mathrm{T}^\mathrm{assoc}$ for $4 &lt; p_\mathrm{T}^\mathrm{e} &lt; 7$ GeV/$c$ and $7 &lt; p_\mathrm{T}^\mathrm{e} &lt; 16$ GeV/$c$ in Pb--Pb collisions in the 0--10% centrality class and pp collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV.
description: The azimuthal-correlation distributions between electrons from the decays of heavy-flavor hadrons and associated charged particles in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV are reported for the 0--10\% and 30--50\% centrality classes. This measurement provides access to the jet-like correlation observables in the heavy-flavor sector in Pb--Pb collisions. The analysis is performed for trigger electrons from heavy-flavor hadron decays with transverse momentum $4 &lt; p_\mathrm{T}^\mathrm{e} &lt; 16~{\mathrm GeV}/c$, considering associated particles within the transverse-momentum range $1 &lt; p_\mathrm{T}^\mathrm{assoc} &lt; 7$ ${\mathrm GeV}/c$, and a pseudorapidity difference of $|\Delta\eta|&lt;1$ between the trigger electron and associated particles. The per-trigger nuclear modification factor ($I_\mathrm{AA}$) is calculated to compare the near- and away-side peak yields to those in pp collisions at $\sqrt{s} = 5.02$ TeV. In 0--10\% central collisions, the $I_\mathrm{AA}$ indicates a hint of enhancement of associated-particle yields with $p_\mathrm{T}&lt;3$ GeV/$c$ on the near side, and a suppression of yields with $p_\mathrm{T}&gt;4$ GeV/$c$ on the away side. The $I_\mathrm{AA}$ for electron triggers from heavy-flavor hadron decays is compared with that for light-flavor and strange-particle triggers to investigate the dependence on different fragmentation processes and parton-medium dynamics, and is found to be the same within uncertainties.
DOI: 10.17182/hepdata.168549.v1/t14
title: "Table 14" of "Medium-induced modification of azimuthal correlations of electrons from heavy-flavor hadron decays with charged particles in Pb-Pb collisions at $\sqrt{s_{\rm{NN}} = 5.02}$ TeV"

description: Per-trigger nuclear modification factor ($I_\mathrm{AA}$) of away-side (AS) $\Delta\varphi$ correlation distribution between electrons from heavy-flavor hadron decays and associated charged particles as a function of $p_\mathrm{T}^\mathrm{assoc}$ for $4 &lt; p_\mathrm{T}^\mathrm{e} &lt; 7$ GeV/$c$ and $7 &lt; p_\mathrm{T}^\mathrm{e} &lt; 16$ GeV/$c$ in Pb--Pb collisions in the 0--10% centrality class and pp collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV.
description: The azimuthal-correlation distributions between electrons from the decays of heavy-flavor hadrons and associated charged particles in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV are reported for the 0--10\% and 30--50\% centrality classes. This measurement provides access to the jet-like correlation observables in the heavy-flavor sector in Pb--Pb collisions. The analysis is performed for trigger electrons from heavy-flavor hadron decays with transverse momentum $4 &lt; p_\mathrm{T}^\mathrm{e} &lt; 16~{\mathrm GeV}/c$, considering associated particles within the transverse-momentum range $1 &lt; p_\mathrm{T}^\mathrm{assoc} &lt; 7$ ${\mathrm GeV}/c$, and a pseudorapidity difference of $|\Delta\eta|&lt;1$ between the trigger electron and associated particles. The per-trigger nuclear modification factor ($I_\mathrm{AA}$) is calculated to compare the near- and away-side peak yields to those in pp collisions at $\sqrt{s} = 5.02$ TeV. In 0--10\% central collisions, the $I_\mathrm{AA}$ indicates a hint of enhancement of associated-particle yields with $p_\mathrm{T}&lt;3$ GeV/$c$ on the near side, and a suppression of yields with $p_\mathrm{T}&gt;4$ GeV/$c$ on the away side. The $I_\mathrm{AA}$ for electron triggers from heavy-flavor hadron decays is compared with that for light-flavor and strange-particle triggers to investigate the dependence on different fragmentation processes and parton-medium dynamics, and is found to be the same within uncertainties.
DOI: 10.17182/hepdata.113508.v1/t1
title: "Figure 3" of "Probing the gluonic structure of the deuteron with $J/\psi$ photoproduction in d+Au ultra-peripheral collisions"

description: Upper - differential cross section as a function of $p^{2}_{T, J/\psi}$ of \jpsi photoproduction in UPCs at $\sqrt{s_{_{\rm NN}}}=200\rm~GeV$. Data for the total diffractive process are shown with solid markers, while data with neutron tagging in the deuteron-going ZDC are shown with open markers. Theoretical predictions based on the saturation model (Color Glass Condensate)[Phys.Rev.C 101 (2020) 1, 015203] and the gluon shadowing model (LTA) [V. Guzey, M. Strikman, E. Kryshen, M. Zhalov] are compared with data, shown as solid lines. Statistical uncertainty is represented by the error bars, and the systematic uncertainty is denoted by the shaded box. For the lower, ratios of total data and models are presented as a function of $-t \approx p^{2}_{T, J/\psi}$. Color bands are statistical uncertainty based on the data only, while systematic uncertainty is indicated by the gray box.
description: RHIC-STAR, Probing the gluonic structure of the deuteron with $J/\psi$ photoproduction in d+Au ultra-peripheral collisions
DOI: 10.17182/hepdata.147196.v1/t1
title: "Figure 2a_0" of "Imaging Shapes of Atomic Nuclei in High-Energy Nuclear Collisions"

description: Data from Figure 2, panel a, Au+Au, 0-0.5% Centrality, 0.2
description: No data abstract available.
DOI: 10.17182/hepdata.147196.v1/t2
title: "Figure 2a_1" of "Imaging Shapes of Atomic Nuclei in High-Energy Nuclear Collisions"

description: Data from Figure 2, panel a, U+U, 0-0.5% Centrality, 0.2
description: No data abstract available.
DOI: 10.17182/hepdata.147196.v1/t3
title: "Figure 2b_0" of "Imaging Shapes of Atomic Nuclei in High-Energy Nuclear Collisions"

description: Data from Figure 2, panel b, Au+Au, 0-0.5% Centrality, 0.2
description: No data abstract available.
DOI: 10.17182/hepdata.147196.v1/t5
title: "Figure 3a" of "Imaging Shapes of Atomic Nuclei in High-Energy Nuclear Collisions"

description: Data from Figure 3, panel a, 0.2
description: No data abstract available.
DOI: 10.17182/hepdata.147196.v1/t6
title: "Figure 3b" of "Imaging Shapes of Atomic Nuclei in High-Energy Nuclear Collisions"

description: Data from Figure 3, panel b, 0.2
description: No data abstract available.
DOI: 10.17182/hepdata.147196.v1/t7
title: "Figure 3c" of "Imaging Shapes of Atomic Nuclei in High-Energy Nuclear Collisions"

description: Data from Figure 3, panel c, 0.2
description: No data abstract available.
DOI: 10.17182/hepdata.147196.v1/t8
title: "Figure 3d" of "Imaging Shapes of Atomic Nuclei in High-Energy Nuclear Collisions"

description: Data from Figure 3, panel d, 0-5% Centrality, 0.2
description: No data abstract available.
DOI: 10.17182/hepdata.147196.v1/t10
title: "Figure 3f" of "Imaging Shapes of Atomic Nuclei in High-Energy Nuclear Collisions"

description: Data from Figure 3, panel f, 0-5% Centrality, 0.2
description: No data abstract available.
DOI: 10.17182/hepdata.147196.v1/t11
title: "Figure 4a_0" of "Imaging Shapes of Atomic Nuclei in High-Energy Nuclear Collisions"

description: Data from Figure 4, panel a, Au+Au, 2subevent method, 0.2
description: No data abstract available.
DOI: 10.17182/hepdata.147196.v1/t12
title: "Figure 4a_1" of "Imaging Shapes of Atomic Nuclei in High-Energy Nuclear Collisions"

description: Data from Figure 4, panel a, U+U, 2subevent method, 0.2
description: No data abstract available.
DOI: 10.17182/hepdata.147196.v1/t13
title: "Figure 4b_0" of "Imaging Shapes of Atomic Nuclei in High-Energy Nuclear Collisions"

description: Data from Figure 4, panel b, Au+Au, 0.2
description: No data abstract available.
DOI: 10.17182/hepdata.147196.v1/t16
title: "Figure 4c_1" of "Imaging Shapes of Atomic Nuclei in High-Energy Nuclear Collisions"

description: Data from Figure 4, panel c, U+U, 0.2
description: No data abstract available.
DOI: 10.17182/hepdata.147196.v1/t17
title: "Figure 4d_0" of "Imaging Shapes of Atomic Nuclei in High-Energy Nuclear Collisions"

description: Data from Figure 4, panel d, Au+Au, 0.2
description: No data abstract available.
DOI: 10.17182/hepdata.147196.v1/t4
title: "Figure 2b_1" of "Imaging Shapes of Atomic Nuclei in High-Energy Nuclear Collisions"

description: Data from Figure 2, panel b, U+U, 0-0.5% Centrality, 0.2
description: No data abstract available.
DOI: 10.17182/hepdata.147196.v1/t9
title: "Figure 3e" of "Imaging Shapes of Atomic Nuclei in High-Energy Nuclear Collisions"

description: Data from Figure 3, panel e, 0-5% Centrality, 0.2
description: No data abstract available.
DOI: 10.17182/hepdata.147196.v1/t14
title: "Figure 4b_1" of "Imaging Shapes of Atomic Nuclei in High-Energy Nuclear Collisions"

description: Data from Figure 4, panel b, U+U, 0.2
description: No data abstract available.
DOI: 10.17182/hepdata.147196.v1/t15
title: "Figure 4c_0" of "Imaging Shapes of Atomic Nuclei in High-Energy Nuclear Collisions"

description: Data from Figure 4, panel c, Au+Au, 0.2
description: No data abstract available.