Abstract

We have studied the transverse-momentum ($p_{\rm T}$) dependence of the inclusive J/$\psi$ production in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV, in three center-of-mass rapidity ($y_{\rm cms}$) regions, down to zero $p_{\rm T}$. Results in the forward and backward rapidity ranges ($2.03 < y_{\rm cms} < 3.53$ and $-4.46 <y_{\rm cms}< -2.96$) are obtained by studying the J/$\psi$ decay to $\mu^+\mu^-$, while the mid-rapidity region ($-1.37 < y_{\rm cms} < 0.43$) is investigated by measuring the ${\rm e}^+{\rm e}^-$ decay channel. The $p_{\rm T}$ dependence of the J/$\psi$ production cross section and nuclear modification factor are presented for each of the rapidity intervals, as well as the J/$\psi$ mean $p_{\rm T}$ values. Forward and mid-rapidity results show a suppression of the J/$\psi$ yield, with respect to pp collisions, which decreases with increasing $p_{\rm T}$. At backward rapidity no significant J/$\psi$ suppression is observed. Theoretical models including a combination of cold nuclear matter effects such as shadowing and partonic energy loss, are in fair agreement with the data, except at forward rapidity and low transverse momentum. The implications of the p-Pb results for the evaluation of cold nuclear matter effects on J/$\psi$ production in Pb-Pb collisions are also discussed.

Highlights

  • These so-called cold nuclear matter (CNM) effects can be investigated by studying charmonium production in proton-nucleus (p-A) collisions as confirmed by the analysis of results obtained by several fixed-target (SPS [3, 4], HERA [5] and Tevatron [6]) and collider (RHIC [7] and LHC [8, 9]) experiments

  • Models [10,11,12] inspired by Quantum ChromoDynamics (QCD) describe charmonium production as a two-step process, with the cc pair created in a hard parton scattering, followed by its evolution into a bound state with specific quantum numbers

  • Parton Distribution Functions (PDFs) are known to be modified in a nuclear environment, information on the dependence of such modifications on the fraction x (Bjorken-x) of the nucleon momentum carried by the gluons and on the four-momentum squared Q2 transferred in the scattering is still limited [13,14,15]

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Summary

Signal extraction

Meer scan to be 2.09 ± 0.07 b for the p-Pb configuration and 2.12 ± 0.07 b for the Pb-p case [43]. The two measurements differ by at most 1% throughout the whole data-taking period and such a value is quadratically added to the luminosity uncertainty. The differential inclusive J/ψ cross sections are shown, in the ranges pT < 10 GeV/c for the dielectron analysis and pT < 15 GeV/c for the dimuon analysis. The pT-integrated cross section was determined, obtaining dσpJP/ψb/dy(−1.37 < ycms < 0.43) = 909 ± 78(stat.) ± 71(syst.)μb. The quoted uncertainties were obtained by performing fits including only statistical (or uncorrelated systematic) uncertainties on differential cross sections. The values obtained in this case are 2.58 ± 0.02(stat.) ± 0.04(syst.) GeV/c and 2.69 ± 0.02(stat.) ± 0.03(syst.) GeV/c, respectively at backward and forward ycms, and differ by ∼ 2σ. The J/ψ nuclear modification factor RpPb is obtained as the ratio of the differential cross sections between proton-nucleus and proton-proton collisions, normalized to APb: RpPb(y, pT)

Since no pp data are available at
Findings
Suppression of

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