Abstract
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 ($|y|<0.8$). 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 $1.5 < p_{\rm T} < 10$ GeV/c in three centrality intervals. No significant centrality dependence of $f_{\rm B}$ 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 $4.5 < p_{\rm T} < 10$ GeV/c is found to be stronger than predicted by most models.
Highlights
PT for inclusive 2.76 TeV in the e+e− decay channel at mid-rapidity (|y| < 0.8)
The production of open beauty hadrons is expected to be sensitive to the density of the medium created in heavy-ion collisions due to the energy loss experienced by the parent parton which hadronizes into the beauty hadron
This energy loss is expected to occur via medium-induced gluon radiation [21, 22] and elastic collisional energy loss processes [23,24,25] and it depends on the QCD Casimir coupling factor of the parton and on the parton mass [26,27,28,29]
Summary
PT for inclusive 2.76 TeV in the e+e− decay channel at mid-rapidity (|y| < 0.8). The pT is significantly smaller than the one observed for pp collisions at the same centre-of-mass energy. 10 GeV/c, The average transverse momentum as a function of the invariant mass mee pT in of e+e− centrality pairs, measured for the pT selected Pb-Pb collisions at range √sNN
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