Abstract
In this contribution we discuss the production of charmonium states in two and three photon fusion processes in nucleus - nucleus collisions at the CERN Large Hadron Collider (LHC) energies. In a previous work we showed that the experimental study of these processes is feasible and they can be used to constrain the theoretical decay widths and give information on the non c−c¯ component of these states. Here we discuss some points which were not addressed in that work.
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