English

Dynamics in near-threshold $J/\psi$ photoproduction

High Energy Physics - Phenomenology 2023-09-14 v2 High Energy Physics - Experiment Nuclear Theory

Abstract

The study of J/ψJ/\psi photoproduction at low energies has consequences for the understanding of multiple aspects of nonperturbative QCD, ranging from mechanical properties of the proton, to the binding inside nuclei, and the existence of hidden-charm pentaquarks. Factorization of the photon-ccˉc \bar c and nucleon dynamics or Vector Meson Dominance are often invoked to justify these studies. Alternatively, open charm intermediate states have been proposed as the dominant mechanism underlying J/ψJ/\psi photoproduction. As the latter violates this factorization, it is important to estimate the relevance of such contributions. We analyse the latest differential and integrated photoproduction cross sections from the GlueX and J/ψJ/\psi-007 experiments. We show that the data can be adequately described by a small number of partial waves, which we parameterize with generic models enforcing low-energy unitarity. The results suggest a nonnegligible contribution from open charm intermediate states. Furthermore, most of the models present an elastic scattering length incompatible with previous extractions based on Vector Meson Dominance, and thus call into question its applicability to heavy mesons. Our results indicate a wide array of physics possibilities that are compatible with present data and need to be disentangled.

Keywords

Cite

@article{arxiv.2305.01449,
  title  = {Dynamics in near-threshold $J/\psi$ photoproduction},
  author = {JPAC Collaboration and D. Winney and C. Fernandez-Ramirez and A. Pilloni and A. N. Hiller Blin and M. Albaladejo and L. Bibrzycki and N. Hammoud and J. Liao and V. Mathieu and G. Montana and R. J. Perry and V. Shastry and W. A. Smith and A. P. Szczepaniak},
  journal= {arXiv preprint arXiv:2305.01449},
  year   = {2023}
}

Comments

15 pages, 7 figures, 2 tables. Version to appear on Phys. Rev. D

R2 v1 2026-06-28T10:23:29.282Z