cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.77790.v1/t19
title: "Table 19" of "Measurements of jet quenching with semi-inclusive hadron+jet distributions in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV"

description: Recoil jet distributions for peripheral Au+Au STAR events after mixed event subtraction as a function of \Delta\phi for p_{T,jet}^{reco,ch} range of 13-33 GeV/c.
description: No data abstract available.
DOI: 10.17182/hepdata.77790.v1/t20
title: "Table 20" of "Measurements of jet quenching with semi-inclusive hadron+jet distributions in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV"

description: Recoil jet distributions after mixed event subtraction as a function of \Delta\phi for p_{T,jet}^{reco,ch} range of 13-33 GeV/c for p+p PYTHIA detector-level simulations.
description: No data abstract available.
DOI: 10.17182/hepdata.77790.v1/t21
title: "Table 21" of "Measurements of jet quenching with semi-inclusive hadron+jet distributions in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV"

description: Recoil jet distributions for central Au+Au STAR events after mixed event subtraction as a function of \Delta\phi for p_{T,jet}^{reco,ch} range of 9-13 GeV/c.
description: No data abstract available.
DOI: 10.17182/hepdata.77790.v1/t22
title: "Table 22" of "Measurements of jet quenching with semi-inclusive hadron+jet distributions in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV"

description: Recoil jet distributions after mixed event subtraction as a function of \Delta\phi for p_{T,jet}^{reco,ch} range of 9-13 GeV/c for p+p PYTHIA detector-level simulations embeded into mixed events from central Au + Au STAR data at the track level.
description: No data abstract available.
DOI: 10.17182/hepdata.77790.v1/t23
title: "Table 23" of "Measurements of jet quenching with semi-inclusive hadron+jet distributions in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV"

description: Recoil jet distributions for central Au+Au STAR events after mixed event subtraction as a function of \Delta\phi for p_{T,jet}^{reco,ch} range of 13-33 GeV/c.
description: No data abstract available.
DOI: 10.17182/hepdata.77790.v1/t24
title: "Table 24" of "Measurements of jet quenching with semi-inclusive hadron+jet distributions in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV"

description: Recoil jet distributions after mixed event subtraction as a function of \Delta\phi for p_{T,jet}^{reco,ch} range of 13-33 GeV/c for p+p PYTHIA detector-level simulations embeded into mixed events from central Au + Au STAR data at the track level.
description: No data abstract available.
DOI: 10.17182/hepdata.77790.v1/t25
title: "Table 25" of "Measurements of jet quenching with semi-inclusive hadron+jet distributions in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV"

description: Fully corrected distributions of Y(p_{t,jet}^{ch}) for central AU + Au collisions at \sqrt{s_{NN}} = 200 GeV, for anti-k_T jets with R = 0.2.
description: No data abstract available.
DOI: 10.17182/hepdata.77790.v1/t26
title: "Table 26" of "Measurements of jet quenching with semi-inclusive hadron+jet distributions in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV"

description: Fully corrected distributions of Y(p_{t,jet}^{ch}) for peripheral AU + Au collisions at \sqrt{s_{NN}} = 200 GeV, for anti-k_T jets with R = 0.2.
description: No data abstract available.
DOI: 10.17182/hepdata.77790.v1/t27
title: "Table 27" of "Measurements of jet quenching with semi-inclusive hadron+jet distributions in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV"

description: Ratio of fully corrected distributions of Y(p_{t,jet}^{ch}) of central to peripheral events for AU + Au collisions at \sqrt{s_{NN}} = 200 GeV, for anti-k_T jets with R = 0.2 (i.e. ratio of Table 17 to Table 18 in this HEPData entry).
description: No data abstract available.
DOI: 10.17182/hepdata.77790.v1/t28
title: "Table 28" of "Measurements of jet quenching with semi-inclusive hadron+jet distributions in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV"

description: Fully corrected distributions of Y(p_{t,jet}^{ch}) for central AU + Au collisions at \sqrt{s_{NN}} = 200 GeV, for anti-k_T jets with R = 0.3.
description: No data abstract available.
DOI: 10.17182/hepdata.77790.v1/t29
title: "Table 29" of "Measurements of jet quenching with semi-inclusive hadron+jet distributions in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV"

description: Fully corrected distributions of Y(p_{t,jet}^{ch}) for peripheral AU + Au collisions at \sqrt{s_{NN}} = 200 GeV, for anti-k_T jets with R = 0.3.
description: No data abstract available.
DOI: 10.17182/hepdata.77790.v1/t30
title: "Table 30" of "Measurements of jet quenching with semi-inclusive hadron+jet distributions in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV"

description: Ratio of fully corrected distributions of Y(p_{t,jet}^{ch}) of central to peripheral events for AU + Au collisions at \sqrt{s_{NN}} = 200 GeV, for anti-k_T jets with R = 0.3 (i.e. ratio of Table 20 to Table 21 in this HEPData entry).
description: No data abstract available.
DOI: 10.17182/hepdata.77790.v1/t31
title: "Table 31" of "Measurements of jet quenching with semi-inclusive hadron+jet distributions in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV"

description: Fully corrected distributions of Y(p_{t,jet}^{ch}) for central AU + Au collisions at \sqrt{s_{NN}} = 200 GeV, for anti-k_T jets with R = 0.4.
description: No data abstract available.
DOI: 10.17182/hepdata.77790.v1/t32
title: "Table 32" of "Measurements of jet quenching with semi-inclusive hadron+jet distributions in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV"

description: Fully corrected distributions of Y(p_{t,jet}^{ch}) for peripheral AU + Au collisions at \sqrt{s_{NN}} = 200 GeV, for anti-k_T jets with R = 0.4.
description: No data abstract available.
DOI: 10.17182/hepdata.77790.v1/t33
title: "Table 33" of "Measurements of jet quenching with semi-inclusive hadron+jet distributions in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV"

description: Ratio of fully corrected distributions of Y(p_{t,jet}^{ch}) of central to peripheral events for AU + Au collisions at \sqrt{s_{NN}} = 200 GeV, for anti-k_T jets with R = 0.4 (i.e. ratio of Table 23 to Table 24 in this HEPData entry).
description: No data abstract available.
DOI: 10.17182/hepdata.77790.v1/t34
title: "Table 34" of "Measurements of jet quenching with semi-inclusive hadron+jet distributions in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV"

description: Fully corrected distributions of Y(p_{t,jet}^{ch}) for central AU + Au collisions at \sqrt{s_{NN}} = 200 GeV, for anti-k_T jets with R = 0.5.
description: No data abstract available.
DOI: 10.17182/hepdata.77790.v1/t35
title: "Table 35" of "Measurements of jet quenching with semi-inclusive hadron+jet distributions in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV"

description: Fully corrected distributions of Y(p_{t,jet}^{ch}) for peripheral AU + Au collisions at \sqrt{s_{NN}} = 200 GeV, for anti-k_T jets with R = 0.5.
description: No data abstract available.
DOI: 10.17182/hepdata.77790.v1/t36
title: "Table 36" of "Measurements of jet quenching with semi-inclusive hadron+jet distributions in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV"

description: Ratio of fully corrected distributions of Y(p_{t,jet}^{ch}) of central to peripheral events for AU + Au collisions at \sqrt{s_{NN}} = 200 GeV, for anti-k_T jets with R = 0.4 (i.e. ratio of Table 26 to Table 27 in this HEPData entry).
description: No data abstract available.
DOI: 10.17182/hepdata.77790.v1/t37
title: "Table 37" of "Measurements of jet quenching with semi-inclusive hadron+jet distributions in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV"

description: Ratio of distributions of Y(p_{T,jet}^{ch}) for R = 0.2 to R = 0.5 in peripheral Au + Au collisions at \sqrt{s_{NN}} = 200 GeV.
description: No data abstract available.
DOI: 10.17182/hepdata.77790.v1/t38
title: "Table 38" of "Measurements of jet quenching with semi-inclusive hadron+jet distributions in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV"

description: Ratio of distributions of Y(p_{T,jet}^{ch}) for R = 0.2 to R = 0.5 in central Au + Au collisions at \sqrt{s_{NN}} = 200 GeV.
description: No data abstract available.
DOI: 10.17182/hepdata.77790.v1/t39
title: "Table 39" of "Measurements of jet quenching with semi-inclusive hadron+jet distributions in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV"

description: Azimuthal distribution of recoil jets, \PSI(\DELTA\phi) in central Au + Au collisions at \sqrt{s_{NN}} = 200 GeV measured at STAR.
description: No data abstract available.
DOI: 10.17182/hepdata.77790.v1/t40
title: "Table 40" of "Measurements of jet quenching with semi-inclusive hadron+jet distributions in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV"

description: Azimuthal distribution of R=0.3 recoil jets, \PSI(\DELTA\phi) in peripheral Au + Au collisions at \sqrt{s_{NN}} = 200 GeV measured at STAR.
description: No data abstract available.
DOI: 10.17182/hepdata.77790.v1/t41
title: "Table 41" of "Measurements of jet quenching with semi-inclusive hadron+jet distributions in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV"

description: Azimuthal distribution of recoil jets, \PSI(\DELTA\phi) in PYTHIA generated pp collisiions at sqrt{s_{NN}} = 200 GeV.
description: No data abstract available.
DOI: 10.17182/hepdata.77790.v1/t42
title: "Table 42" of "Measurements of jet quenching with semi-inclusive hadron+jet distributions in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV"

description: Azimuthal distribution of recoil jets, \PSI(\DELTA\phi) in PYTHIA generated pp collisiions embedded in central Au + Au Mixed Events at sqrt{s_{NN}} = 200 GeV.
description: No data abstract available.
DOI: 10.17182/hepdata.77815.v1/t1
title: "Table 1" of "Test of lepton universality with $B^{0} \rightarrow K^{*0}\ell^{+}\ell^{-}$ decays"

description: Distributions of the $R(K^{*0})$ delta log-likelihood, $-(\ln L - \ln L_{best})$, for the three trigger categories combined in the low-q2 bin ($0.045 &lt; q^2 &lt; 1.1$ GeV$^{2}/c^4$).
description: CERN-LHC. A test of lepton universality, performed by measuring the ratio of the branching fractions of the $B^{0} \rightarrow K^{*0}\mu^{+}\mu^{-}$ and $B^{0} \rightarrow K^{*0}e^{+}e^{-}$ decays, $R_{K^{*0}}$, is presented. The $K^* 892^{0}$ meson is reconstructed in the final state $K^{+}\pi^{-}$, which is required to have an invariant mass within $100\mathrm{\,MeV/}c^2$ of the known $K^{*}(892)^{0}$ mass. The analysis is performed using proton-proton collision data, corresponding to an integrated luminosity of about $3\mathrm{\,fb}^{-1}$, collected by the LHCb experiment at centre-of-mass energies of $7$ and $8\mathrm{\,TeV}$. The ratio is measured in two regions of the dilepton invariant mass squared, $q^{2}$, to be $$R_{K^{*0}} = \begin{cases} 0.66~^{+~0.11}_{-~0.07}\mathrm{\,(stat)} \pm 0.03\mathrm{\,(syst)} &\textrm{for } 0.045 &lt; q^{2} &lt; 1.1~\mathrm{\,GeV^2/}c^4, \\ 0.69~^{+~0.11}_{-~0.07}\mathrm{\,(stat)} \pm 0.05\mathrm{\,(syst)} & \textrm{for } 1.1\phantom{00} &lt; q^{2} &lt; 6.0~\mathrm{\,GeV^2/}c^4 . \end{cases}$$ The corresponding 95.4% confidence level intervals are [0.52, 0.89] and [0.53, 0.94]. The results, which represent the most precise measurements of $R_{K^{*0}}$ to date, are compatible with the Standard Model expectations at the level of 2.1-2.3 and 2.4-2.5 standard deviations in the two $q^{2}$ regions, respectively. This record presents the combined distributions of the $R_{K^{*0}}$ delta log-likelihood (for the three electron trigger categories detailed in the paper) in the two regions of dilepton invariant mass squared.
DOI: 10.17182/hepdata.77815.v1/t2
title: "Table 2" of "Test of lepton universality with $B^{0} \rightarrow K^{*0}\ell^{+}\ell^{-}$ decays"

description: Distributions of the $R(K^{*0})$ delta log-likelihood, $-(\ln L - \ln L_{best})$, for the three trigger categories combined in the central-q2 bin ($1.1 &lt; q^2 &lt; 6.0$ GeV$^{2}/c^4$).
description: CERN-LHC. A test of lepton universality, performed by measuring the ratio of the branching fractions of the $B^{0} \rightarrow K^{*0}\mu^{+}\mu^{-}$ and $B^{0} \rightarrow K^{*0}e^{+}e^{-}$ decays, $R_{K^{*0}}$, is presented. The $K^* 892^{0}$ meson is reconstructed in the final state $K^{+}\pi^{-}$, which is required to have an invariant mass within $100\mathrm{\,MeV/}c^2$ of the known $K^{*}(892)^{0}$ mass. The analysis is performed using proton-proton collision data, corresponding to an integrated luminosity of about $3\mathrm{\,fb}^{-1}$, collected by the LHCb experiment at centre-of-mass energies of $7$ and $8\mathrm{\,TeV}$. The ratio is measured in two regions of the dilepton invariant mass squared, $q^{2}$, to be $$R_{K^{*0}} = \begin{cases} 0.66~^{+~0.11}_{-~0.07}\mathrm{\,(stat)} \pm 0.03\mathrm{\,(syst)} &\textrm{for } 0.045 &lt; q^{2} &lt; 1.1~\mathrm{\,GeV^2/}c^4, \\ 0.69~^{+~0.11}_{-~0.07}\mathrm{\,(stat)} \pm 0.05\mathrm{\,(syst)} & \textrm{for } 1.1\phantom{00} &lt; q^{2} &lt; 6.0~\mathrm{\,GeV^2/}c^4 . \end{cases}$$ The corresponding 95.4% confidence level intervals are [0.52, 0.89] and [0.53, 0.94]. The results, which represent the most precise measurements of $R_{K^{*0}}$ to date, are compatible with the Standard Model expectations at the level of 2.1-2.3 and 2.4-2.5 standard deviations in the two $q^{2}$ regions, respectively. This record presents the combined distributions of the $R_{K^{*0}}$ delta log-likelihood (for the three electron trigger categories detailed in the paper) in the two regions of dilepton invariant mass squared.
DOI: 10.17182/hepdata.77817.v1/t1
title: "Table 1" of "Measurement of the production of high-$p_{\rm T}$ electrons from heavy-flavour hadron decays in Pb-Pb collisions at $\mathbf{\sqrt{\it s_{\rm{NN}}}}$ = 2.76 TeV"

description: Pb-Pb collision centrality 0-10%.
description: CERN-LHC. Electrons from heavy-flavour hadron decays (charm and beauty) were measured with the ALICE detector in Pb-Pb collisions at a centre-of-mass of energy $\sqrt{s_{\rm NN}}=2.76$ TeV. The transverse momentum ($p_{\rm T}$) differential production yields at mid-rapidity were used to calculate the nuclear modification factor $R_{\rm AA}$ in the interval $3&lt;~p_{\rm T}&lt;~ 18$ GeV/$c$. The $R_{\rm AA}$ shows a strong suppression compared to binary scaling of pp collisions at the same energy (up to a factor of 4) in the 10% most central Pb-Pb collisions. There is a centrality trend of suppression, and a weaker suppression (down to a factor of 2) in semi-peripheral (50-80%) collisions is observed.
DOI: 10.17182/hepdata.77817.v1/t2
title: "Table 2" of "Measurement of the production of high-$p_{\rm T}$ electrons from heavy-flavour hadron decays in Pb-Pb collisions at $\mathbf{\sqrt{\it s_{\rm{NN}}}}$ = 2.76 TeV"

description: Pb-Pb collision centrality 10-20%.
description: CERN-LHC. Electrons from heavy-flavour hadron decays (charm and beauty) were measured with the ALICE detector in Pb-Pb collisions at a centre-of-mass of energy $\sqrt{s_{\rm NN}}=2.76$ TeV. The transverse momentum ($p_{\rm T}$) differential production yields at mid-rapidity were used to calculate the nuclear modification factor $R_{\rm AA}$ in the interval $3&lt;~p_{\rm T}&lt;~ 18$ GeV/$c$. The $R_{\rm AA}$ shows a strong suppression compared to binary scaling of pp collisions at the same energy (up to a factor of 4) in the 10% most central Pb-Pb collisions. There is a centrality trend of suppression, and a weaker suppression (down to a factor of 2) in semi-peripheral (50-80%) collisions is observed.
DOI: 10.17182/hepdata.77817.v1/t3
title: "Table 3" of "Measurement of the production of high-$p_{\rm T}$ electrons from heavy-flavour hadron decays in Pb-Pb collisions at $\mathbf{\sqrt{\it s_{\rm{NN}}}}$ = 2.76 TeV"

description: Pb-Pb collision centrality 20-30%.
description: CERN-LHC. Electrons from heavy-flavour hadron decays (charm and beauty) were measured with the ALICE detector in Pb-Pb collisions at a centre-of-mass of energy $\sqrt{s_{\rm NN}}=2.76$ TeV. The transverse momentum ($p_{\rm T}$) differential production yields at mid-rapidity were used to calculate the nuclear modification factor $R_{\rm AA}$ in the interval $3&lt;~p_{\rm T}&lt;~ 18$ GeV/$c$. The $R_{\rm AA}$ shows a strong suppression compared to binary scaling of pp collisions at the same energy (up to a factor of 4) in the 10% most central Pb-Pb collisions. There is a centrality trend of suppression, and a weaker suppression (down to a factor of 2) in semi-peripheral (50-80%) collisions is observed.
DOI: 10.17182/hepdata.77817.v1/t4
title: "Table 4" of "Measurement of the production of high-$p_{\rm T}$ electrons from heavy-flavour hadron decays in Pb-Pb collisions at $\mathbf{\sqrt{\it s_{\rm{NN}}}}$ = 2.76 TeV"

description: Pb-Pb collision centrality 30-40%.
description: CERN-LHC. Electrons from heavy-flavour hadron decays (charm and beauty) were measured with the ALICE detector in Pb-Pb collisions at a centre-of-mass of energy $\sqrt{s_{\rm NN}}=2.76$ TeV. The transverse momentum ($p_{\rm T}$) differential production yields at mid-rapidity were used to calculate the nuclear modification factor $R_{\rm AA}$ in the interval $3&lt;~p_{\rm T}&lt;~ 18$ GeV/$c$. The $R_{\rm AA}$ shows a strong suppression compared to binary scaling of pp collisions at the same energy (up to a factor of 4) in the 10% most central Pb-Pb collisions. There is a centrality trend of suppression, and a weaker suppression (down to a factor of 2) in semi-peripheral (50-80%) collisions is observed.
DOI: 10.17182/hepdata.77817.v1/t5
title: "Table 5" of "Measurement of the production of high-$p_{\rm T}$ electrons from heavy-flavour hadron decays in Pb-Pb collisions at $\mathbf{\sqrt{\it s_{\rm{NN}}}}$ = 2.76 TeV"

description: Pb-Pb collision centrality 40-50%.
description: CERN-LHC. Electrons from heavy-flavour hadron decays (charm and beauty) were measured with the ALICE detector in Pb-Pb collisions at a centre-of-mass of energy $\sqrt{s_{\rm NN}}=2.76$ TeV. The transverse momentum ($p_{\rm T}$) differential production yields at mid-rapidity were used to calculate the nuclear modification factor $R_{\rm AA}$ in the interval $3&lt;~p_{\rm T}&lt;~ 18$ GeV/$c$. The $R_{\rm AA}$ shows a strong suppression compared to binary scaling of pp collisions at the same energy (up to a factor of 4) in the 10% most central Pb-Pb collisions. There is a centrality trend of suppression, and a weaker suppression (down to a factor of 2) in semi-peripheral (50-80%) collisions is observed.
DOI: 10.17182/hepdata.77817.v1/t6
title: "Table 6" of "Measurement of the production of high-$p_{\rm T}$ electrons from heavy-flavour hadron decays in Pb-Pb collisions at $\mathbf{\sqrt{\it s_{\rm{NN}}}}$ = 2.76 TeV"

description: Pb-Pb collision centrality 50-80%.
description: CERN-LHC. Electrons from heavy-flavour hadron decays (charm and beauty) were measured with the ALICE detector in Pb-Pb collisions at a centre-of-mass of energy $\sqrt{s_{\rm NN}}=2.76$ TeV. The transverse momentum ($p_{\rm T}$) differential production yields at mid-rapidity were used to calculate the nuclear modification factor $R_{\rm AA}$ in the interval $3&lt;~p_{\rm T}&lt;~ 18$ GeV/$c$. The $R_{\rm AA}$ shows a strong suppression compared to binary scaling of pp collisions at the same energy (up to a factor of 4) in the 10% most central Pb-Pb collisions. There is a centrality trend of suppression, and a weaker suppression (down to a factor of 2) in semi-peripheral (50-80%) collisions is observed.
DOI: 10.17182/hepdata.77817.v1/t10
title: "Table 10" of "Measurement of the production of high-$p_{\rm T}$ electrons from heavy-flavour hadron decays in Pb-Pb collisions at $\mathbf{\sqrt{\it s_{\rm{NN}}}}$ = 2.76 TeV"

description: Pb-Pb collision centrality 30-40%.
description: CERN-LHC. Electrons from heavy-flavour hadron decays (charm and beauty) were measured with the ALICE detector in Pb-Pb collisions at a centre-of-mass of energy $\sqrt{s_{\rm NN}}=2.76$ TeV. The transverse momentum ($p_{\rm T}$) differential production yields at mid-rapidity were used to calculate the nuclear modification factor $R_{\rm AA}$ in the interval $3&lt;~p_{\rm T}&lt;~ 18$ GeV/$c$. The $R_{\rm AA}$ shows a strong suppression compared to binary scaling of pp collisions at the same energy (up to a factor of 4) in the 10% most central Pb-Pb collisions. There is a centrality trend of suppression, and a weaker suppression (down to a factor of 2) in semi-peripheral (50-80%) collisions is observed.
DOI: 10.17182/hepdata.77817.v1/t11
title: "Table 11" of "Measurement of the production of high-$p_{\rm T}$ electrons from heavy-flavour hadron decays in Pb-Pb collisions at $\mathbf{\sqrt{\it s_{\rm{NN}}}}$ = 2.76 TeV"

description: Pb-Pb collision centrality 40-50%.
description: CERN-LHC. Electrons from heavy-flavour hadron decays (charm and beauty) were measured with the ALICE detector in Pb-Pb collisions at a centre-of-mass of energy $\sqrt{s_{\rm NN}}=2.76$ TeV. The transverse momentum ($p_{\rm T}$) differential production yields at mid-rapidity were used to calculate the nuclear modification factor $R_{\rm AA}$ in the interval $3&lt;~p_{\rm T}&lt;~ 18$ GeV/$c$. The $R_{\rm AA}$ shows a strong suppression compared to binary scaling of pp collisions at the same energy (up to a factor of 4) in the 10% most central Pb-Pb collisions. There is a centrality trend of suppression, and a weaker suppression (down to a factor of 2) in semi-peripheral (50-80%) collisions is observed.
DOI: 10.17182/hepdata.77817.v1/t12
title: "Table 12" of "Measurement of the production of high-$p_{\rm T}$ electrons from heavy-flavour hadron decays in Pb-Pb collisions at $\mathbf{\sqrt{\it s_{\rm{NN}}}}$ = 2.76 TeV"

description: Pb-Pb collision centrality 50-80%.
description: CERN-LHC. Electrons from heavy-flavour hadron decays (charm and beauty) were measured with the ALICE detector in Pb-Pb collisions at a centre-of-mass of energy $\sqrt{s_{\rm NN}}=2.76$ TeV. The transverse momentum ($p_{\rm T}$) differential production yields at mid-rapidity were used to calculate the nuclear modification factor $R_{\rm AA}$ in the interval $3&lt;~p_{\rm T}&lt;~ 18$ GeV/$c$. The $R_{\rm AA}$ shows a strong suppression compared to binary scaling of pp collisions at the same energy (up to a factor of 4) in the 10% most central Pb-Pb collisions. There is a centrality trend of suppression, and a weaker suppression (down to a factor of 2) in semi-peripheral (50-80%) collisions is observed.
DOI: 10.17182/hepdata.77817.v1/t7
title: "Table 7" of "Measurement of the production of high-$p_{\rm T}$ electrons from heavy-flavour hadron decays in Pb-Pb collisions at $\mathbf{\sqrt{\it s_{\rm{NN}}}}$ = 2.76 TeV"

description: Pb-Pb collision centrality 0-10%.
description: CERN-LHC. Electrons from heavy-flavour hadron decays (charm and beauty) were measured with the ALICE detector in Pb-Pb collisions at a centre-of-mass of energy $\sqrt{s_{\rm NN}}=2.76$ TeV. The transverse momentum ($p_{\rm T}$) differential production yields at mid-rapidity were used to calculate the nuclear modification factor $R_{\rm AA}$ in the interval $3&lt;~p_{\rm T}&lt;~ 18$ GeV/$c$. The $R_{\rm AA}$ shows a strong suppression compared to binary scaling of pp collisions at the same energy (up to a factor of 4) in the 10% most central Pb-Pb collisions. There is a centrality trend of suppression, and a weaker suppression (down to a factor of 2) in semi-peripheral (50-80%) collisions is observed.