Abstract

We calculate the centrality dependence for coherent photoproduction of very low- p T J / ψ at Relativistic Heavy Ion Collider (RHIC) and Large Hadron Collider (LHC) energies within the impact parameter-dependent saturated color dipole model. By using the large equivalent photon fluxes, we present the differential cross-section of very low- p T J / ψ produced by coherent photonuclear in peripheral heavy ion collisions. The numerical results demonstrate that our calculation agrees with J / ψ data in peripheral heavy ion collisions at Relativistic Heavy Ion Collider (RHIC) energies.

Highlights

  • The Relativistic Heavy Ion Collider (RHIC) and Large Hadron Collider (LHC) are the most powerful collider for the central and noncentral heavy ion collisions, offering a unique opportunity to study fundamental aspects of quantum electrodynamics (QED) and quantum chromodynamics (QCD)

  • A significant excess of J/ψ yield at very low transverse momenta has been observed by the ALICE cpoffilffilffiaffiffibffiffi oration in peripheral hadronic Pb-Pb collisions with sNN = 2:76 TeV at forward rapidity [30], and by thpe ffiSffiffiTffiffiffiAffi R collaboration in hadronic Au-Au pcoffiffiffilffilffiiffiffisions with sNN = 200 GeV and U-U collisions with sNN = 193 GeV at midrapidity [31, 32], that cannot be explained within the hadronic J/ψ production modified by the cold and hot medium effects

  • In order to present our results in a way that can be compared with STAR data from RHIC, we will study the invariant yield of very low-pT J/ψ production as the following: B

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Summary

Introduction

The Relativistic Heavy Ion Collider (RHIC) and Large Hadron Collider (LHC) are the most powerful collider for the central and noncentral heavy ion collisions, offering a unique opportunity to study fundamental aspects of quantum electrodynamics (QED) and quantum chromodynamics (QCD). A significant excess of J/ψ yield at very low transverse momenta has been observed by the ALICE cpoffilffilffiaffiffibffiffi oration in peripheral hadronic Pb-Pb collisions with sNN = 2:76 TeV at forward rapidity [30], and by thpe ffiSffiffiTffiffiffiAffi R collaboration in hadronic Au-Au pcoffiffiffilffilffiiffiffisions with sNN = 200 GeV and U-U collisions with sNN = 193 GeV at midrapidity [31, 32], that cannot be explained within the hadronic J/ψ production modified by the cold and hot medium effects It indicates that the significant excess maybe originated from the coherent photoproduction in hadronic heavy ion collisions (b < 2R).

General Formalism
Numerical Results
Conclusions
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