cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.133216.v1/t11
title: "Figure-4-Tabel-1" of "Search for the Chiral Magnetic Effect in Au+Au collisions at $\sqrt{s_{_{\rm{NN}}}}=27$ GeV with the STAR forward Event Plane Detectors"

description: This dataset corresponds to Figure 4, the \Delta\gamma_{112}multiply N_{part} and scaled by v_2 estimated by tpc (\Psi_2) in the paper
description: No data abstract available.
DOI: 10.17182/hepdata.133216.v1/t12
title: "Figure-4-Tabel-2" of "Search for the Chiral Magnetic Effect in Au+Au collisions at $\sqrt{s_{_{\rm{NN}}}}=27$ GeV with the STAR forward Event Plane Detectors"

description: This dataset corresponds to Figure 4, the \Delta\gamma_{112}multiply N_{part} and scaled by v_2 estimated by epd (\Psi_2) in the paper
description: No data abstract available.
DOI: 10.17182/hepdata.133216.v1/t8
title: "Figure-3-Tabel-3" of "Search for the Chiral Magnetic Effect in Au+Au collisions at $\sqrt{s_{_{\rm{NN}}}}=27$ GeV with the STAR forward Event Plane Detectors"

description: This dataset corresponds to Figure 3, the \Delta\gamma_{1111}multiply N_{part} value estimated by epd (\Psi_1) in the paper
description: No data abstract available.
DOI: 10.17182/hepdata.133216.v1/t9
title: "Figure-3-Tabel-4" of "Search for the Chiral Magnetic Effect in Au+Au collisions at $\sqrt{s_{_{\rm{NN}}}}=27$ GeV with the STAR forward Event Plane Detectors"

description: This dataset corresponds to Figure 3, the ratio between \Delta\gamma_{1111} (by epd \Psi_1) and \Delta\gamma(112) (by tpc \Psi_2) in the paper
description: No data abstract available.
DOI: 10.17182/hepdata.133216.v1/t13
title: "Figure-4-Tabel-3" of "Search for the Chiral Magnetic Effect in Au+Au collisions at $\sqrt{s_{_{\rm{NN}}}}=27$ GeV with the STAR forward Event Plane Detectors"

description: This dataset corresponds to Figure 4, the \Delta\gamma_{1111}multiply N_{part} and scaled by v_2 estimated by epd (\Psi_1) in the paper
description: No data abstract available.
DOI: 10.17182/hepdata.133216.v1/t14
title: "Figure-4-Tabel-4" of "Search for the Chiral Magnetic Effect in Au+Au collisions at $\sqrt{s_{_{\rm{NN}}}}=27$ GeV with the STAR forward Event Plane Detectors"

description: This dataset corresponds to Figure 4, the ratio between \Delta\gamma_{1111} scaled by v_{211} (by epd \Psi_1) and \Delta\gamma(112) scaled by v_2 (by tpc \Psi_2) in the paper
description: No data abstract available.
DOI: 10.17182/hepdata.133216.v1/t15
title: "Figure-4-Tabel-5" of "Search for the Chiral Magnetic Effect in Au+Au collisions at $\sqrt{s_{_{\rm{NN}}}}=27$ GeV with the STAR forward Event Plane Detectors"

description: This dataset corresponds to Figure 4, the ratio between \Delta\gamma_{1111} scaled by v_{211} (by epd \Psi_1) and \Delta\gamma(112) scaled by v_2 (by epd \Psi_2) in the paper
description: No data abstract available.
DOI: 10.5061/dryad.b5mkkwhs3
title: Data from: Catalytic promotion of transition-metal-doped graphene cathodes in Li-CO<sub>2</sub> batteries

description: The Li-CO2 battery is a promising energy storage system with impressive
 theoretical specific energy and discharge capacity. Graphene-based
 single-atom catalysts (SACs) provide high surface area and long-term
 electrochemical reactivity and stability, making SACs among the most
 promising cathode catalysts for these batteries. However, current Li-CO2
 systems have high reaction barriers, slowing the reaction and greatly
 increasing the overpotential. Improvement of the discharge/charge
 energetics requires atomic-level innovations in cathode design, such as
 alterations to the catalyst chemical structure. In this paper, we propose
 enhancing the SAC by using a Ti metal center, which is found to deliver
 the highest electrochemical Li + CO2 activity among 3d transition metal
 candidates. Furthermore, we propose cathode surface coating with ionic
 liquids, since these environments promote the formation of reaction
 intermediates in the electrochemical conversion process. Our work provides
 insights to optimize electrode design for high-performance Li-CO2
 batteries, which can open new avenues to recycle greenhouse gases and
 achieve enhanced renewable energy storage. Inputs to calculations,
 containing all density functional theory calculation parameters, are
 provided.
description: # Data from: Catalytic promotion of transition-metal-doped graphene
 cathodes in Li-CO~2~ batteries Dataset DOI:
 [10.5061/dryad.b5mkkwhs3](10.5061/dryad.b5mkkwhs3) ## Description of the
 data and file structure Input files used to evaluate catalytic effect of
 various graphene-based cathode catalysts toward the proposed Li-CO2
 battery reaction, as well as brief investigation of the effect of metal
 substrates, ligands, and ionic liquid on catalytic performance. ### Files
 and variables #### File: CatalyticPromotionMar2025.tar.gz
 **Description:** Contains input files for Quantum ESPRESSO and JDFTx
 calculations.
DOI: 10.17182/hepdata.134246.v1/t1
title: "Table 1" of "Dielectron production at midrapidity at low transverse momentum in peripheral and semi-peripheral Pb$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV"

description: Differential $e^+e^-$ yield in 50--70\% Pb--Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV as a function of $m_{\rm ee}$ for $p_{\rm T,ee} &lt; 0.1$ GeV/$c$. Electrons are measured within $|\eta_{\rm e}| &lt; 0.8$ and $p_{\rm T,e} &gt; 0.2$ GeV/$c$. The quoted upper limits correspond to a 90% confidence level.
description: No data abstract available.
DOI: 10.17182/hepdata.134246.v1/t2
title: "Table 2" of "Dielectron production at midrapidity at low transverse momentum in peripheral and semi-peripheral Pb$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV"

description: Differential $e^+e^-$ yield in 70--90\% Pb--Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV as a function of $m_{\rm ee}$ for $p_{\rm T,ee} &lt; 0.1$ GeV/$c$. Electrons are measured within $|\eta_{\rm e}| &lt; 0.8$ and $p_{\rm T,e} &gt; 0.2$ GeV/$c$.
description: No data abstract available.
DOI: 10.17182/hepdata.134246.v1/t10
title: "Table 10" of "Dielectron production at midrapidity at low transverse momentum in peripheral and semi-peripheral Pb$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV"

description: Differential excess $e^+e^-$ yield in 70--90\% Pb--Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV as a function of $p^{2}_{\rm T,ee}$ for 1.1 $&lt; m_{\rm ee} &lt; 2.7$ GeV/$c^{\rm 2}$. Electrons are measured within $|\eta_{\rm e}| &lt; 0.8$ and $p_{\rm T,e} &gt; 0.2$ GeV/$c$.
description: No data abstract available.
DOI: 10.17182/hepdata.134246.v1/t3
title: "Table 3" of "Dielectron production at midrapidity at low transverse momentum in peripheral and semi-peripheral Pb$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV"

description: Differential excess $e^+e^-$ yield in 50--70\% Pb--Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV as a function of $m_{\rm ee}$ for $p_{\rm T,ee} &lt; 0.1$ GeV/$c$. Electrons are measured within $|\eta_{\rm e}| &lt; 0.8$ and $p_{\rm T,e} &gt; 0.2$ GeV/$c$. The quoted upper limits correspond to a 90% confidence level.
description: No data abstract available.
DOI: 10.17182/hepdata.134246.v1/t4
title: "Table 4" of "Dielectron production at midrapidity at low transverse momentum in peripheral and semi-peripheral Pb$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV"

description: Differential excess $e^+e^-$ yield in 70--90\% Pb--Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV as a function of $m_{\rm ee}$ for $p_{\rm T,ee} &lt; 0.1$ GeV/$c$. Electrons are measured within $|\eta_{\rm e}| &lt; 0.8$ and $p_{\rm T,e} &gt; 0.2$ GeV/$c$.
description: No data abstract available.
DOI: 10.17182/hepdata.134246.v1/t5
title: "Table 5" of "Dielectron production at midrapidity at low transverse momentum in peripheral and semi-peripheral Pb$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV"

description: Differential $e^+e^-$ yield in 70--90\% Pb--Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV as a function of $p_{\rm T,ee}$ for 0.4 $&lt; m_{\rm ee} &lt; 0.7$ GeV/$c^{\rm 2}$. Electrons are measured within $|\eta_{\rm e}| &lt; 0.8$ and $p_{\rm T,e} &gt; 0.2$ GeV/$c$.
description: No data abstract available.
DOI: 10.17182/hepdata.134246.v1/t6
title: "Table 6" of "Dielectron production at midrapidity at low transverse momentum in peripheral and semi-peripheral Pb$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV"

description: Differential $e^+e^-$ yield in 70--90\% Pb--Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV as a function of $p_{\rm T,ee}$ for 0.7 $&lt; m_{\rm ee} &lt; 1.1$ GeV/$c^{\rm 2}$. Electrons are measured within $|\eta_{\rm e}| &lt; 0.8$ and $p_{\rm T,e} &gt; 0.2$ GeV/$c$. The quoted upper limits correspond to a 90% confidence level.
description: No data abstract available.
DOI: 10.17182/hepdata.134246.v1/t7
title: "Table 7" of "Dielectron production at midrapidity at low transverse momentum in peripheral and semi-peripheral Pb$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV"

description: Differential $e^+e^-$ yield in 70--90\% Pb--Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV as a function of $p_{\rm T,ee}$ for 1.1 $&lt; m_{\rm ee} &lt; 2.7$ GeV/$c^{\rm 2}$. Electrons are measured within $|\eta_{\rm e}| &lt; 0.8$ and $p_{\rm T,e} &gt; 0.2$ GeV/$c$. The quoted upper limits correspond to a 90% confidence level.
description: No data abstract available.
DOI: 10.17182/hepdata.134246.v1/t8
title: "Table 8" of "Dielectron production at midrapidity at low transverse momentum in peripheral and semi-peripheral Pb$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV"

description: Differential excess $e^+e^-$ yield in 70--90\% Pb--Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV as a function of $p^{2}_{\rm T,ee}$ for 0.4 $&lt; m_{\rm ee} &lt; 0.7$ GeV/$c^{\rm 2}$. Electrons are measured within $|\eta_{\rm e}| &lt; 0.8$ and $p_{\rm T,e} &gt; 0.2$ GeV/$c$. The quoted upper limits correspond to a 90% confidence level.
description: No data abstract available.
DOI: 10.17182/hepdata.134246.v1/t9
title: "Table 9" of "Dielectron production at midrapidity at low transverse momentum in peripheral and semi-peripheral Pb$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV"

description: Differential excess $e^+e^-$ yield in 70--90\% Pb--Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV as a function of $p^{2}_{\rm T,ee}$ for 0.7 $&lt; m_{\rm ee} &lt; 1.1$ GeV/$c^{\rm 2}$. Electrons are measured within $|\eta_{\rm e}| &lt; 0.8$ and $p_{\rm T,e} &gt; 0.2$ GeV/$c$. The quoted upper limits correspond to a 90% confidence level.
description: No data abstract available.
DOI: 10.17182/hepdata.68881.v1/t1
title: "Table 1" of "Inclusive, prompt and non-prompt J/$\psi$ production at mid-rapidity in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV"

description: The average transverse momentum $\langle p_{\rm T} \rangle$ of inclusive J/$\psi$ measured at mid-rapidity in centrality selected Pb-Pb collisions as a function of the number of participants.
description: CERN-LHC. The transverse momentum $p_{\rm T}$ dependence of the nuclear modification factor $R_{\rm AA}$ and the centrality dependence of the average transverse momentum $\langle p_{\rm T} \rangle$ for inclusive J/$\psi$ have been measured with ALICE for Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV in the e+e- decay channel at mid-rapidity ($|y|$ &lt; 0.8). The $\langle p_{\rm T} \rangle$ is significantly smaller than the one observed for pp collisions at the same centre-of-mass energy. Consistently, an increase of $R_{\rm AA}$ is observed towards low $p_{\rm T}$. These observations might be indicative of a sizable contribution of charm quark coalescence to the J/$\psi$ production. Additionally, the fraction of non-prompt J/$\psi$ from beauty hadron decays, $f_{\rm B}$, has been determined in the region 1.5 &lt; $p_{\rm T}$ &lt; 10 GeV/$c$ in three centrality intervals. No significant centrality dependence of fB is observed. Finally, the $R_{\rm AA}$ of non-prompt J/$\psi$ is discussed and compared with model predictions. The nuclear modification in the region 4.5 &lt; $p_{\rm T}$ &lt; 10 GeV/$c$ is found to be stronger than predicted by most models.
DOI: 10.17182/hepdata.68881.v1/t2
title: "Table 2" of "Inclusive, prompt and non-prompt J/$\psi$ production at mid-rapidity in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV"

description: The average transverse momentum squared $\langle p_{\rm T}^{2} \rangle$ of inclusive J/$\psi$ measured at mid-rapidity in centrality selected Pb-Pb collisions as a function of the number of participants.
description: CERN-LHC. The transverse momentum $p_{\rm T}$ dependence of the nuclear modification factor $R_{\rm AA}$ and the centrality dependence of the average transverse momentum $\langle p_{\rm T} \rangle$ for inclusive J/$\psi$ have been measured with ALICE for Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV in the e+e- decay channel at mid-rapidity ($|y|$ &lt; 0.8). The $\langle p_{\rm T} \rangle$ is significantly smaller than the one observed for pp collisions at the same centre-of-mass energy. Consistently, an increase of $R_{\rm AA}$ is observed towards low $p_{\rm T}$. These observations might be indicative of a sizable contribution of charm quark coalescence to the J/$\psi$ production. Additionally, the fraction of non-prompt J/$\psi$ from beauty hadron decays, $f_{\rm B}$, has been determined in the region 1.5 &lt; $p_{\rm T}$ &lt; 10 GeV/$c$ in three centrality intervals. No significant centrality dependence of fB is observed. Finally, the $R_{\rm AA}$ of non-prompt J/$\psi$ is discussed and compared with model predictions. The nuclear modification in the region 4.5 &lt; $p_{\rm T}$ &lt; 10 GeV/$c$ is found to be stronger than predicted by most models.
DOI: 10.17182/hepdata.68881.v1/t3
title: "Table 3" of "Inclusive, prompt and non-prompt J/$\psi$ production at mid-rapidity in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV"

description: The ratio $\langle p_{\rm T}^{2} \rangle_{\rm AA} / \langle p_{\rm T}^{2} \rangle_{\rm pp}$ of inclusive J/$\psi$ measured at mid-rapidity in centrality selected Pb-Pb collisions as a function of the number of participants.
description: CERN-LHC. The transverse momentum $p_{\rm T}$ dependence of the nuclear modification factor $R_{\rm AA}$ and the centrality dependence of the average transverse momentum $\langle p_{\rm T} \rangle$ for inclusive J/$\psi$ have been measured with ALICE for Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV in the e+e- decay channel at mid-rapidity ($|y|$ &lt; 0.8). The $\langle p_{\rm T} \rangle$ is significantly smaller than the one observed for pp collisions at the same centre-of-mass energy. Consistently, an increase of $R_{\rm AA}$ is observed towards low $p_{\rm T}$. These observations might be indicative of a sizable contribution of charm quark coalescence to the J/$\psi$ production. Additionally, the fraction of non-prompt J/$\psi$ from beauty hadron decays, $f_{\rm B}$, has been determined in the region 1.5 &lt; $p_{\rm T}$ &lt; 10 GeV/$c$ in three centrality intervals. No significant centrality dependence of fB is observed. Finally, the $R_{\rm AA}$ of non-prompt J/$\psi$ is discussed and compared with model predictions. The nuclear modification in the region 4.5 &lt; $p_{\rm T}$ &lt; 10 GeV/$c$ is found to be stronger than predicted by most models.
DOI: 10.17182/hepdata.68881.v1/t4
title: "Table 4" of "Inclusive, prompt and non-prompt J/$\psi$ production at mid-rapidity in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV"

description: The nuclear modification factor $R_{\rm AA}$ of inclusive J/$\psi$ measured at mid-rapidity in Pb-Pb collisions (0-40 % most central) as a function of the transverse momentum $p_{\rm T}$.
description: CERN-LHC. The transverse momentum $p_{\rm T}$ dependence of the nuclear modification factor $R_{\rm AA}$ and the centrality dependence of the average transverse momentum $\langle p_{\rm T} \rangle$ for inclusive J/$\psi$ have been measured with ALICE for Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV in the e+e- decay channel at mid-rapidity ($|y|$ &lt; 0.8). The $\langle p_{\rm T} \rangle$ is significantly smaller than the one observed for pp collisions at the same centre-of-mass energy. Consistently, an increase of $R_{\rm AA}$ is observed towards low $p_{\rm T}$. These observations might be indicative of a sizable contribution of charm quark coalescence to the J/$\psi$ production. Additionally, the fraction of non-prompt J/$\psi$ from beauty hadron decays, $f_{\rm B}$, has been determined in the region 1.5 &lt; $p_{\rm T}$ &lt; 10 GeV/$c$ in three centrality intervals. No significant centrality dependence of fB is observed. Finally, the $R_{\rm AA}$ of non-prompt J/$\psi$ is discussed and compared with model predictions. The nuclear modification in the region 4.5 &lt; $p_{\rm T}$ &lt; 10 GeV/$c$ is found to be stronger than predicted by most models.
DOI: 10.17182/hepdata.68881.v1/t5
title: "Table 5" of "Inclusive, prompt and non-prompt J/$\psi$ production at mid-rapidity in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV"

description: The nuclear modification factor $R_{\rm AA}$ of inclusive J/$\psi$ measured at mid-rapidity in Pb-Pb collisions (0-50 % most central) as a function of the transverse momentum $p_{\rm T}$.
description: CERN-LHC. The transverse momentum $p_{\rm T}$ dependence of the nuclear modification factor $R_{\rm AA}$ and the centrality dependence of the average transverse momentum $\langle p_{\rm T} \rangle$ for inclusive J/$\psi$ have been measured with ALICE for Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV in the e+e- decay channel at mid-rapidity ($|y|$ &lt; 0.8). The $\langle p_{\rm T} \rangle$ is significantly smaller than the one observed for pp collisions at the same centre-of-mass energy. Consistently, an increase of $R_{\rm AA}$ is observed towards low $p_{\rm T}$. These observations might be indicative of a sizable contribution of charm quark coalescence to the J/$\psi$ production. Additionally, the fraction of non-prompt J/$\psi$ from beauty hadron decays, $f_{\rm B}$, has been determined in the region 1.5 &lt; $p_{\rm T}$ &lt; 10 GeV/$c$ in three centrality intervals. No significant centrality dependence of fB is observed. Finally, the $R_{\rm AA}$ of non-prompt J/$\psi$ is discussed and compared with model predictions. The nuclear modification in the region 4.5 &lt; $p_{\rm T}$ &lt; 10 GeV/$c$ is found to be stronger than predicted by most models.
DOI: 10.17182/hepdata.68881.v1/t7
title: "Table 7" of "Inclusive, prompt and non-prompt J/$\psi$ production at mid-rapidity in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV"

description: The fraction of J/$\psi$ from beauty hadron decays $f_{\rm B}$ at mid-rapidity as a function of transverse momentum $p_{\rm T}$.
description: CERN-LHC. The transverse momentum $p_{\rm T}$ dependence of the nuclear modification factor $R_{\rm AA}$ and the centrality dependence of the average transverse momentum $\langle p_{\rm T} \rangle$ for inclusive J/$\psi$ have been measured with ALICE for Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV in the e+e- decay channel at mid-rapidity ($|y|$ &lt; 0.8). The $\langle p_{\rm T} \rangle$ is significantly smaller than the one observed for pp collisions at the same centre-of-mass energy. Consistently, an increase of $R_{\rm AA}$ is observed towards low $p_{\rm T}$. These observations might be indicative of a sizable contribution of charm quark coalescence to the J/$\psi$ production. Additionally, the fraction of non-prompt J/$\psi$ from beauty hadron decays, $f_{\rm B}$, has been determined in the region 1.5 &lt; $p_{\rm T}$ &lt; 10 GeV/$c$ in three centrality intervals. No significant centrality dependence of fB is observed. Finally, the $R_{\rm AA}$ of non-prompt J/$\psi$ is discussed and compared with model predictions. The nuclear modification in the region 4.5 &lt; $p_{\rm T}$ &lt; 10 GeV/$c$ is found to be stronger than predicted by most models.
DOI: 10.17182/hepdata.68881.v1/t8
title: "Table 8" of "Inclusive, prompt and non-prompt J/$\psi$ production at mid-rapidity in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV"

description: The nuclear modification factor $R_{\rm AA}$ of non-prompt J/$\psi$ at mid-rapidity as a function of transverse momentum $p_{\rm T}$.
description: CERN-LHC. The transverse momentum $p_{\rm T}$ dependence of the nuclear modification factor $R_{\rm AA}$ and the centrality dependence of the average transverse momentum $\langle p_{\rm T} \rangle$ for inclusive J/$\psi$ have been measured with ALICE for Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV in the e+e- decay channel at mid-rapidity ($|y|$ &lt; 0.8). The $\langle p_{\rm T} \rangle$ is significantly smaller than the one observed for pp collisions at the same centre-of-mass energy. Consistently, an increase of $R_{\rm AA}$ is observed towards low $p_{\rm T}$. These observations might be indicative of a sizable contribution of charm quark coalescence to the J/$\psi$ production. Additionally, the fraction of non-prompt J/$\psi$ from beauty hadron decays, $f_{\rm B}$, has been determined in the region 1.5 &lt; $p_{\rm T}$ &lt; 10 GeV/$c$ in three centrality intervals. No significant centrality dependence of fB is observed. Finally, the $R_{\rm AA}$ of non-prompt J/$\psi$ is discussed and compared with model predictions. The nuclear modification in the region 4.5 &lt; $p_{\rm T}$ &lt; 10 GeV/$c$ is found to be stronger than predicted by most models.
DOI: 10.17182/hepdata.68881.v1/t6
title: "Table 6" of "Inclusive, prompt and non-prompt J/$\psi$ production at mid-rapidity in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV"

description: The fraction of J/$\psi$ from beauty hadron decays $f_{\rm
 B}$ at mid-rapidity in the $p_{\rm T}$ interval 1.5 - 10 GeV/$c$ as a function of the number of participants.
description: CERN-LHC. The transverse momentum $p_{\rm T}$ dependence of the nuclear modification factor $R_{\rm AA}$ and the centrality dependence of the average transverse momentum $\langle p_{\rm T} \rangle$ for inclusive J/$\psi$ have been measured with ALICE for Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV in the e+e- decay channel at mid-rapidity ($|y|$ &lt; 0.8). The $\langle p_{\rm T} \rangle$ is significantly smaller than the one observed for pp collisions at the same centre-of-mass energy. Consistently, an increase of $R_{\rm AA}$ is observed towards low $p_{\rm T}$. These observations might be indicative of a sizable contribution of charm quark coalescence to the J/$\psi$ production. Additionally, the fraction of non-prompt J/$\psi$ from beauty hadron decays, $f_{\rm B}$, has been determined in the region 1.5 &lt; $p_{\rm T}$ &lt; 10 GeV/$c$ in three centrality intervals. No significant centrality dependence of fB is observed. Finally, the $R_{\rm AA}$ of non-prompt J/$\psi$ is discussed and compared with model predictions. The nuclear modification in the region 4.5 &lt; $p_{\rm T}$ &lt; 10 GeV/$c$ is found to be stronger than predicted by most models.