arXiv:1103.5516 [nucl-th]AbstractReferencesReviewsResources
$J/Ψ$-nuclear bound states
K. Tsushima, D. H. Lu, G. Krein, A. W. Thomas
Published 2011-03-29, updated 2011-06-11Version 2
$J/\Psi$-nuclear bound state energies are calculated for a range of nuclei by solving the Proca (Klein-Gordon) equation. Critical input for the calculations, namely the medium-modified $D$ and $D^*$ meson masses, as well as the nucleon density distributions in nuclei, are obtained from the quark-meson coupling model. The attractive potential originates from the $D$ and $D^*$ meson loops in the $J/\Psi$ self-energy in nuclear medium. It appears that $J/\Psi$-nuclear bound states should produce a clear experimental signature provided that the $J/\Psi$ meson is produced in recoilless kinematics.
Comments: 11 pages, 4 figures, 1 table, to appear in Phys. Rev. C. Further comments on the width of J/Psi-nuclear states, effective Lagrangians, and new references
Journal: Phys.Rev.C83:065208,2011
Keywords: nuclear bound state energies, clear experimental signature, nucleon density distributions, nuclear medium, meson loops
Tags: journal article
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