cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.142077.v1/t9
title: "Figure 7a-2" of "Transverse-Momentum Dependence of the J/psi Nuclear Modification in d+Au Collisions at sqrt(s_NN)=200 GeV"

description: $J/\psi$ invariant yield as a function of $p_T$ for each centrality for −2.2 &lt; $y$ &lt; −1.2. The type C systematic uncertainty for each distribution is given as a percentage in the legend. Type A represents uncertainties that are uncorrelated from point to point, Type B represents uncertainties that are correlated from point to point, and Type C represents uncertainties in the overall normalization.
description: We present measured $J/\psi$ production rates in $d$+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV over a broad range of transverse momentum ($p_T$ = 0–14 GeV/$c$) and rapidity (−2.2 &lt; y &lt; 2.2). We construct the nuclear-modification factor $R_{dAu}$ for these kinematics and as a function of collision centrality (related to impact parameter for the $R_{dAu}$ collision). We find that the modification is largest for collisions with small impact parameters, and observe a suppression ($R_{dAu}$ &lt; 1) for $p_T$ &lt; 4 GeV/$c$ at positive rapidities. At negative rapidity we observe a suppression for $p_T$ &lt; 2 GeV/$c$ then an enhancement ($R_{dAu}$ &gt; 1) for pT &gt; 2 GeV/$c$. The observed enhancement at negative rapidity has implications for the observed modification in heavy-ion collisions at high $p_T$.
DOI: 10.17182/hepdata.142077.v1/t12
title: "Figure 7b-1" of "Transverse-Momentum Dependence of the J/psi Nuclear Modification in d+Au Collisions at sqrt(s_NN)=200 GeV"

description: $J/\psi$ invariant yield as a function of $p_T$ for each centrality for −2.2 &lt; $y$ &lt; −1.2. The type C systematic uncertainty for each distribution is given as a percentage in the legend. Type A represents uncertainties that are uncorrelated from point to point, Type B represents uncertainties that are correlated from point to point, and Type C represents uncertainties in the overall normalization.
description: We present measured $J/\psi$ production rates in $d$+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV over a broad range of transverse momentum ($p_T$ = 0–14 GeV/$c$) and rapidity (−2.2 &lt; y &lt; 2.2). We construct the nuclear-modification factor $R_{dAu}$ for these kinematics and as a function of collision centrality (related to impact parameter for the $R_{dAu}$ collision). We find that the modification is largest for collisions with small impact parameters, and observe a suppression ($R_{dAu}$ &lt; 1) for $p_T$ &lt; 4 GeV/$c$ at positive rapidities. At negative rapidity we observe a suppression for $p_T$ &lt; 2 GeV/$c$ then an enhancement ($R_{dAu}$ &gt; 1) for pT &gt; 2 GeV/$c$. The observed enhancement at negative rapidity has implications for the observed modification in heavy-ion collisions at high $p_T$.
DOI: 10.17182/hepdata.142077.v1/t13
title: "Figure 7b-2" of "Transverse-Momentum Dependence of the J/psi Nuclear Modification in d+Au Collisions at sqrt(s_NN)=200 GeV"

description: $J/\psi$ invariant yield as a function of $p_T$ for each centrality for −2.2 &lt; $y$ &lt; −1.2. The type C systematic uncertainty for each distribution is given as a percentage in the legend. Type A represents uncertainties that are uncorrelated from point to point, Type B represents uncertainties that are correlated from point to point, and Type C represents uncertainties in the overall normalization.
description: We present measured $J/\psi$ production rates in $d$+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV over a broad range of transverse momentum ($p_T$ = 0–14 GeV/$c$) and rapidity (−2.2 &lt; y &lt; 2.2). We construct the nuclear-modification factor $R_{dAu}$ for these kinematics and as a function of collision centrality (related to impact parameter for the $R_{dAu}$ collision). We find that the modification is largest for collisions with small impact parameters, and observe a suppression ($R_{dAu}$ &lt; 1) for $p_T$ &lt; 4 GeV/$c$ at positive rapidities. At negative rapidity we observe a suppression for $p_T$ &lt; 2 GeV/$c$ then an enhancement ($R_{dAu}$ &gt; 1) for pT &gt; 2 GeV/$c$. The observed enhancement at negative rapidity has implications for the observed modification in heavy-ion collisions at high $p_T$.
DOI: 10.17182/hepdata.142077.v1/t14
title: "Figure 7b-3" of "Transverse-Momentum Dependence of the J/psi Nuclear Modification in d+Au Collisions at sqrt(s_NN)=200 GeV"

description: $J/\psi$ invariant yield as a function of $p_T$ for each centrality for −2.2 &lt; $y$ &lt; −1.2. The type C systematic uncertainty for each distribution is given as a percentage in the legend. Type A represents uncertainties that are uncorrelated from point to point, Type B represents uncertainties that are correlated from point to point, and Type C represents uncertainties in the overall normalization.
description: We present measured $J/\psi$ production rates in $d$+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV over a broad range of transverse momentum ($p_T$ = 0–14 GeV/$c$) and rapidity (−2.2 &lt; y &lt; 2.2). We construct the nuclear-modification factor $R_{dAu}$ for these kinematics and as a function of collision centrality (related to impact parameter for the $R_{dAu}$ collision). We find that the modification is largest for collisions with small impact parameters, and observe a suppression ($R_{dAu}$ &lt; 1) for $p_T$ &lt; 4 GeV/$c$ at positive rapidities. At negative rapidity we observe a suppression for $p_T$ &lt; 2 GeV/$c$ then an enhancement ($R_{dAu}$ &gt; 1) for pT &gt; 2 GeV/$c$. The observed enhancement at negative rapidity has implications for the observed modification in heavy-ion collisions at high $p_T$.
DOI: 10.17182/hepdata.142077.v1/t15
title: "Figure 7b-4" of "Transverse-Momentum Dependence of the J/psi Nuclear Modification in d+Au Collisions at sqrt(s_NN)=200 GeV"

description: $J/\psi$ invariant yield as a function of $p_T$ for each centrality for −2.2 &lt; $y$ &lt; −1.2. The type C systematic uncertainty for each distribution is given as a percentage in the legend. Type A represents uncertainties that are uncorrelated from point to point, Type B represents uncertainties that are correlated from point to point, and Type C represents uncertainties in the overall normalization.
description: We present measured $J/\psi$ production rates in $d$+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV over a broad range of transverse momentum ($p_T$ = 0–14 GeV/$c$) and rapidity (−2.2 &lt; y &lt; 2.2). We construct the nuclear-modification factor $R_{dAu}$ for these kinematics and as a function of collision centrality (related to impact parameter for the $R_{dAu}$ collision). We find that the modification is largest for collisions with small impact parameters, and observe a suppression ($R_{dAu}$ &lt; 1) for $p_T$ &lt; 4 GeV/$c$ at positive rapidities. At negative rapidity we observe a suppression for $p_T$ &lt; 2 GeV/$c$ then an enhancement ($R_{dAu}$ &gt; 1) for pT &gt; 2 GeV/$c$. The observed enhancement at negative rapidity has implications for the observed modification in heavy-ion collisions at high $p_T$.
DOI: 10.17182/hepdata.142077.v1/t16
title: "Figure 9a" of "Transverse-Momentum Dependence of the J/psi Nuclear Modification in d+Au Collisions at sqrt(s_NN)=200 GeV"

description: $J/\psi$ nuclear modification factor, $R_{dAu}$, as a function of $p_T$ for (a) backward rapidity 0–100% centrality integrated $d$+Au collisions. Type A represents uncertainties that are uncorrelated from point to point, Type B represents uncertainties that are correlated from point to point, and Type C represents uncertainties in the overall normalization.
description: We present measured $J/\psi$ production rates in $d$+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV over a broad range of transverse momentum ($p_T$ = 0–14 GeV/$c$) and rapidity (−2.2 &lt; y &lt; 2.2). We construct the nuclear-modification factor $R_{dAu}$ for these kinematics and as a function of collision centrality (related to impact parameter for the $R_{dAu}$ collision). We find that the modification is largest for collisions with small impact parameters, and observe a suppression ($R_{dAu}$ &lt; 1) for $p_T$ &lt; 4 GeV/$c$ at positive rapidities. At negative rapidity we observe a suppression for $p_T$ &lt; 2 GeV/$c$ then an enhancement ($R_{dAu}$ &gt; 1) for pT &gt; 2 GeV/$c$. The observed enhancement at negative rapidity has implications for the observed modification in heavy-ion collisions at high $p_T$.
DOI: 10.17182/hepdata.142077.v1/t17
title: "Figure 9b" of "Transverse-Momentum Dependence of the J/psi Nuclear Modification in d+Au Collisions at sqrt(s_NN)=200 GeV"

description: $J/\psi$ nuclear modification factor, $R_{dAu}$, as a function of $p_T$ for (b) midrapidity 0–100% centrality integrated $d$+Au collisions. Type A represents uncertainties that are uncorrelated from point to point, Type B represents uncertainties that are correlated from point to point, and Type C represents uncertainties in the overall normalization.
description: We present measured $J/\psi$ production rates in $d$+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV over a broad range of transverse momentum ($p_T$ = 0–14 GeV/$c$) and rapidity (−2.2 &lt; y &lt; 2.2). We construct the nuclear-modification factor $R_{dAu}$ for these kinematics and as a function of collision centrality (related to impact parameter for the $R_{dAu}$ collision). We find that the modification is largest for collisions with small impact parameters, and observe a suppression ($R_{dAu}$ &lt; 1) for $p_T$ &lt; 4 GeV/$c$ at positive rapidities. At negative rapidity we observe a suppression for $p_T$ &lt; 2 GeV/$c$ then an enhancement ($R_{dAu}$ &gt; 1) for pT &gt; 2 GeV/$c$. The observed enhancement at negative rapidity has implications for the observed modification in heavy-ion collisions at high $p_T$.
DOI: 10.17182/hepdata.142077.v1/t18
title: "Figure 9c" of "Transverse-Momentum Dependence of the J/psi Nuclear Modification in d+Au Collisions at sqrt(s_NN)=200 GeV"

description: $J/\psi$ nuclear modification factor, $R_{dAu}$, as a function of $p_T$ for (c) forward rapidity 0–100% centrality integrated $d$+Au collisions. Type A represents uncertainties that are uncorrelated from point to point, Type B represents uncertainties that are correlated from point to point, and Type C represents uncertainties in the overall normalization.
description: We present measured $J/\psi$ production rates in $d$+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV over a broad range of transverse momentum ($p_T$ = 0–14 GeV/$c$) and rapidity (−2.2 &lt; y &lt; 2.2). We construct the nuclear-modification factor $R_{dAu}$ for these kinematics and as a function of collision centrality (related to impact parameter for the $R_{dAu}$ collision). We find that the modification is largest for collisions with small impact parameters, and observe a suppression ($R_{dAu}$ &lt; 1) for $p_T$ &lt; 4 GeV/$c$ at positive rapidities. At negative rapidity we observe a suppression for $p_T$ &lt; 2 GeV/$c$ then an enhancement ($R_{dAu}$ &gt; 1) for pT &gt; 2 GeV/$c$. The observed enhancement at negative rapidity has implications for the observed modification in heavy-ion collisions at high $p_T$.
DOI: 10.17182/hepdata.142077.v1/t19
title: "Figure 11a" of "Transverse-Momentum Dependence of the J/psi Nuclear Modification in d+Au Collisions at sqrt(s_NN)=200 GeV"

description: $J/\psi$ —&gt; $\mu^+\mu^-$ $R_{dAu}$, as a function of $p_T$ for a) central events at −2.2 &lt; $y$ &lt; −1.2. Type A represents uncertainties that are uncorrelated from point to point, Type B represents uncertainties that are correlated from point to point, and Type C represents uncertainties in the overall normalization.
description: We present measured $J/\psi$ production rates in $d$+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV over a broad range of transverse momentum ($p_T$ = 0–14 GeV/$c$) and rapidity (−2.2 &lt; y &lt; 2.2). We construct the nuclear-modification factor $R_{dAu}$ for these kinematics and as a function of collision centrality (related to impact parameter for the $R_{dAu}$ collision). We find that the modification is largest for collisions with small impact parameters, and observe a suppression ($R_{dAu}$ &lt; 1) for $p_T$ &lt; 4 GeV/$c$ at positive rapidities. At negative rapidity we observe a suppression for $p_T$ &lt; 2 GeV/$c$ then an enhancement ($R_{dAu}$ &gt; 1) for pT &gt; 2 GeV/$c$. The observed enhancement at negative rapidity has implications for the observed modification in heavy-ion collisions at high $p_T$.
DOI: 10.17182/hepdata.142077.v1/t20
title: "Figure 11b" of "Transverse-Momentum Dependence of the J/psi Nuclear Modification in d+Au Collisions at sqrt(s_NN)=200 GeV"

description: $J/\psi$ —&gt; $\mu^+\mu^-$ $R_{dAu}$, as a function of $p_T$ for b) midcentral events at −2.2 &lt; $y$ &lt; −1.2. Type A represents uncertainties that are uncorrelated from point to point, Type B represents uncertainties that are correlated from point to point, and Type C represents uncertainties in the overall normalization.
description: We present measured $J/\psi$ production rates in $d$+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV over a broad range of transverse momentum ($p_T$ = 0–14 GeV/$c$) and rapidity (−2.2 &lt; y &lt; 2.2). We construct the nuclear-modification factor $R_{dAu}$ for these kinematics and as a function of collision centrality (related to impact parameter for the $R_{dAu}$ collision). We find that the modification is largest for collisions with small impact parameters, and observe a suppression ($R_{dAu}$ &lt; 1) for $p_T$ &lt; 4 GeV/$c$ at positive rapidities. At negative rapidity we observe a suppression for $p_T$ &lt; 2 GeV/$c$ then an enhancement ($R_{dAu}$ &gt; 1) for pT &gt; 2 GeV/$c$. The observed enhancement at negative rapidity has implications for the observed modification in heavy-ion collisions at high $p_T$.
DOI: 10.17182/hepdata.142077.v1/t22
title: "Figure 11d" of "Transverse-Momentum Dependence of the J/psi Nuclear Modification in d+Au Collisions at sqrt(s_NN)=200 GeV"

description: $J/\psi$ —&gt; $\mu^+\mu^-$ $R_{dAu}$, as a function of $p_T$ for d) peripheral events at −2.2 &lt; $y$ &lt; −1.2. The 60–88% $R_{dAu}$ point at $p_T$ = 5.75 GeV/$c$ has been left off the figure, as it is above the plotted range and has very large uncertainties, however it is included in the table. Type A represents uncertainties that are uncorrelated from point to point, Type B represents uncertainties that are correlated from point to point, and Type C represents uncertainties in the overall normalization.
description: We present measured $J/\psi$ production rates in $d$+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV over a broad range of transverse momentum ($p_T$ = 0–14 GeV/$c$) and rapidity (−2.2 &lt; y &lt; 2.2). We construct the nuclear-modification factor $R_{dAu}$ for these kinematics and as a function of collision centrality (related to impact parameter for the $R_{dAu}$ collision). We find that the modification is largest for collisions with small impact parameters, and observe a suppression ($R_{dAu}$ &lt; 1) for $p_T$ &lt; 4 GeV/$c$ at positive rapidities. At negative rapidity we observe a suppression for $p_T$ &lt; 2 GeV/$c$ then an enhancement ($R_{dAu}$ &gt; 1) for pT &gt; 2 GeV/$c$. The observed enhancement at negative rapidity has implications for the observed modification in heavy-ion collisions at high $p_T$.
DOI: 10.17182/hepdata.142077.v1/t21
title: "Figure 11c" of "Transverse-Momentum Dependence of the J/psi Nuclear Modification in d+Au Collisions at sqrt(s_NN)=200 GeV"

description: $J/\psi$ —&gt; $\mu^+\mu^-$ $R_{dAu}$, as a function of $p_T$ for c) midperipheral events at −2.2 &lt; $y$ &lt; −1.2. Type A represents uncertainties that are uncorrelated from point to point, Type B represents uncertainties that are correlated from point to point, and Type C represents uncertainties in the overall normalization.
description: We present measured $J/\psi$ production rates in $d$+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV over a broad range of transverse momentum ($p_T$ = 0–14 GeV/$c$) and rapidity (−2.2 &lt; y &lt; 2.2). We construct the nuclear-modification factor $R_{dAu}$ for these kinematics and as a function of collision centrality (related to impact parameter for the $R_{dAu}$ collision). We find that the modification is largest for collisions with small impact parameters, and observe a suppression ($R_{dAu}$ &lt; 1) for $p_T$ &lt; 4 GeV/$c$ at positive rapidities. At negative rapidity we observe a suppression for $p_T$ &lt; 2 GeV/$c$ then an enhancement ($R_{dAu}$ &gt; 1) for pT &gt; 2 GeV/$c$. The observed enhancement at negative rapidity has implications for the observed modification in heavy-ion collisions at high $p_T$.
DOI: 10.17182/hepdata.142077.v1/t23
title: "Figure 12" of "Transverse-Momentum Dependence of the J/psi Nuclear Modification in d+Au Collisions at sqrt(s_NN)=200 GeV"

description: $J/\psi$ —&gt; $e^+e^-$ $R_{dAu}$, as a function of $p_T$ for a) central, b) midcentral, c) midperipheral, and d) peripheral events at $|y|$ &lt; 0.35. Type A represents uncertainties that are uncorrelated from point to point, Type B represents uncertainties that are correlated from point to point, and Type C represents uncertainties in the overall normalization.
description: We present measured $J/\psi$ production rates in $d$+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV over a broad range of transverse momentum ($p_T$ = 0–14 GeV/$c$) and rapidity (−2.2 &lt; y &lt; 2.2). We construct the nuclear-modification factor $R_{dAu}$ for these kinematics and as a function of collision centrality (related to impact parameter for the $R_{dAu}$ collision). We find that the modification is largest for collisions with small impact parameters, and observe a suppression ($R_{dAu}$ &lt; 1) for $p_T$ &lt; 4 GeV/$c$ at positive rapidities. At negative rapidity we observe a suppression for $p_T$ &lt; 2 GeV/$c$ then an enhancement ($R_{dAu}$ &gt; 1) for pT &gt; 2 GeV/$c$. The observed enhancement at negative rapidity has implications for the observed modification in heavy-ion collisions at high $p_T$.
DOI: 10.17182/hepdata.142077.v1/t24
title: "Figure 13a" of "Transverse-Momentum Dependence of the J/psi Nuclear Modification in d+Au Collisions at sqrt(s_NN)=200 GeV"

description: $J/\psi$ —&gt; $\mu^+\mu^-$ $R_{dAu}$, as a function of $p_T$ for a) central events at 1.2 &lt; $y$ &lt; 2.2. Type A represents uncertainties that are uncorrelated from point to point, Type B represents uncertainties that are correlated from point to point, and Type C represents uncertainties in the overall normalization.
description: We present measured $J/\psi$ production rates in $d$+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV over a broad range of transverse momentum ($p_T$ = 0–14 GeV/$c$) and rapidity (−2.2 &lt; y &lt; 2.2). We construct the nuclear-modification factor $R_{dAu}$ for these kinematics and as a function of collision centrality (related to impact parameter for the $R_{dAu}$ collision). We find that the modification is largest for collisions with small impact parameters, and observe a suppression ($R_{dAu}$ &lt; 1) for $p_T$ &lt; 4 GeV/$c$ at positive rapidities. At negative rapidity we observe a suppression for $p_T$ &lt; 2 GeV/$c$ then an enhancement ($R_{dAu}$ &gt; 1) for pT &gt; 2 GeV/$c$. The observed enhancement at negative rapidity has implications for the observed modification in heavy-ion collisions at high $p_T$.
DOI: 10.17182/hepdata.142077.v1/t25
title: "Figure 13b" of "Transverse-Momentum Dependence of the J/psi Nuclear Modification in d+Au Collisions at sqrt(s_NN)=200 GeV"

description: $J/\psi$ —&gt; $\mu^+\mu^-$ $R_{dAu}$, as a function of $p_T$ for b) midcentral events at 1.2 &lt; $y$ &lt; 2.2. Type A represents uncertainties that are uncorrelated from point to point, Type B represents uncertainties that are correlated from point to point, and Type C represents uncertainties in the overall normalization.
description: We present measured $J/\psi$ production rates in $d$+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV over a broad range of transverse momentum ($p_T$ = 0–14 GeV/$c$) and rapidity (−2.2 &lt; y &lt; 2.2). We construct the nuclear-modification factor $R_{dAu}$ for these kinematics and as a function of collision centrality (related to impact parameter for the $R_{dAu}$ collision). We find that the modification is largest for collisions with small impact parameters, and observe a suppression ($R_{dAu}$ &lt; 1) for $p_T$ &lt; 4 GeV/$c$ at positive rapidities. At negative rapidity we observe a suppression for $p_T$ &lt; 2 GeV/$c$ then an enhancement ($R_{dAu}$ &gt; 1) for pT &gt; 2 GeV/$c$. The observed enhancement at negative rapidity has implications for the observed modification in heavy-ion collisions at high $p_T$.
DOI: 10.17182/hepdata.142077.v1/t26
title: "Figure 13c" of "Transverse-Momentum Dependence of the J/psi Nuclear Modification in d+Au Collisions at sqrt(s_NN)=200 GeV"

description: $J/\psi$ —&gt; $\mu^+\mu^-$ $R_{dAu}$, as a function of $p_T$ for c) midperipheral events at 1.2 &lt; $y$ &lt; 2.2. Type A represents uncertainties that are uncorrelated from point to point, Type B represents uncertainties that are correlated from point to point, and Type C represents uncertainties in the overall normalization.
description: We present measured $J/\psi$ production rates in $d$+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV over a broad range of transverse momentum ($p_T$ = 0–14 GeV/$c$) and rapidity (−2.2 &lt; y &lt; 2.2). We construct the nuclear-modification factor $R_{dAu}$ for these kinematics and as a function of collision centrality (related to impact parameter for the $R_{dAu}$ collision). We find that the modification is largest for collisions with small impact parameters, and observe a suppression ($R_{dAu}$ &lt; 1) for $p_T$ &lt; 4 GeV/$c$ at positive rapidities. At negative rapidity we observe a suppression for $p_T$ &lt; 2 GeV/$c$ then an enhancement ($R_{dAu}$ &gt; 1) for pT &gt; 2 GeV/$c$. The observed enhancement at negative rapidity has implications for the observed modification in heavy-ion collisions at high $p_T$.
DOI: 10.17182/hepdata.142077.v1/t27
title: "Figure 13d" of "Transverse-Momentum Dependence of the J/psi Nuclear Modification in d+Au Collisions at sqrt(s_NN)=200 GeV"

description: $J/\psi$ —&gt; $\mu^+\mu^-$ $R_{dAu}$, as a function of $p_T$ for d) peripheral events at 1.2 &lt; $y$ &lt; 2.2. Type A represents uncertainties that are uncorrelated from point to point, Type B represents uncertainties that are correlated from point to point, and Type C represents uncertainties in the overall normalization.
description: We present measured $J/\psi$ production rates in $d$+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV over a broad range of transverse momentum ($p_T$ = 0–14 GeV/$c$) and rapidity (−2.2 &lt; y &lt; 2.2). We construct the nuclear-modification factor $R_{dAu}$ for these kinematics and as a function of collision centrality (related to impact parameter for the $R_{dAu}$ collision). We find that the modification is largest for collisions with small impact parameters, and observe a suppression ($R_{dAu}$ &lt; 1) for $p_T$ &lt; 4 GeV/$c$ at positive rapidities. At negative rapidity we observe a suppression for $p_T$ &lt; 2 GeV/$c$ then an enhancement ($R_{dAu}$ &gt; 1) for pT &gt; 2 GeV/$c$. The observed enhancement at negative rapidity has implications for the observed modification in heavy-ion collisions at high $p_T$.