Abstract

We present a measurement of inclusive J/$\psi$ production in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV as a function of the centrality of the collision, as estimated from the energy deposited in the Zero Degree Calorimeters. The measurement is performed with the ALICE detector down to zero transverse momentum, $p_{\rm T}$, in the backward ($-4.46 < y_{\rm cms} < -2.96$) and forward ($2.03 < y_{\rm cms} < 3.53$) rapidity intervals in the dimuon decay channel and in the mid-rapidity region ($-1.37 < y_{\rm cms} < 0.43$) in the dielectron decay channel. The backward and forward rapidity intervals correspond to the Pb-going and p-going direction, respectively. The $p_{\rm T}$-differential J/$\psi$ production cross section at backward and forward rapidity is measured for several centrality classes, together with the corresponding average $p_{\rm T}$ and $p^2_{\rm T}$ values. The nuclear modification factor, $Q_{\rm pPb}$, is presented as a function of centrality for the three rapidity intervals, and, additionally, at backward and forward rapidity, as a function of $p_{\rm T}$ for several centrality classes. At mid- and forward rapidity, the J/$\psi$ yield is suppressed up to 40% compared to that in pp interactions scaled by the number of binary collisions. The degree of suppression increases towards central p-Pb collisions at forward rapidity, and with decreasing $p_{\rm T}$ of the J/$\psi$. At backward rapidity, the $Q_{\rm pPb}$ is compatible with unity within the total uncertainties, with an increasing trend from peripheral to central p-Pb collisions.

Highlights

  • SNN = 5.02 TeV as a function of the centrality of the collision, as estimated from the energy deposited in the Zero Degree Calorimeters

  • NJ/ψ→l+l− (A × ) · ∆y where NJ/ψ→l+l− is the raw number of J/ψ mesons decaying into dileptons for a given centrality class, rapidity and parameterised as f (pT) range, NMB is the number of Minimum Bias (MB) events for the given centrality class, A× is the acceptance times efficiency described in section 3 and 4 and ∆y and ∆pT are the widths of the rapidity and pT intervals, respectively

  • The pT-integrated J/ψ cross sections are reported in table 3 for the three rapidity intervals as a function of centrality expressed in percentiles of the non-single diffractive p-Pb cross section

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Summary

Detectors and data sets

The ALICE apparatus and its performance are described in detail in ref. [50] and ref. [51], respectively. The average number of binary nucleon collisions ( Ncoll ) or the average nuclear overlap function ( TpPb ) for a given centrality class, defined by a selected range of energy deposited in the Pb-remnant side of ZN, is obtained using the hybrid method described in ref. The values of Npart for a given ZN-energy class, noted as ZN class in the following, were calculated by scaling the MB value of the number of participant nucleons, NpMarBt , by the ratio of the average charged-particle multiplicities measured at mid-rapidity for the considered ZN-energy event classes to the corresponding value in MB collisions. The values of Ncmolullt and TpmPublt used in this analysis are reported in table 1, together with their uncertainties

Analysis in the dimuon decay channel
Analysis in the dielectron decay channel
Results
Conclusions
Deceased II Also at
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