Variation of hadron masses in finite nuclei

Details Variation of hadron masses in finite nuclei Variation of hadron masses in finite nuclei

1996-11-29

arxiv.org/abs/nucl-th/9612001v1

Phys.Rev.C55:2637-2648,1997

Physics

Nuclear Physics

Nuclear Theory

34 pages, 13 postscript figures, uses epsfig.sty

Scientific paper

10.1103/PhysRevC.55.2637

The quark-meson coupling model, based on a mean-field description of non-overlapping nucleon bags bound by the self-consistent exchange of $\sigma$, $\omega$ and $\rho$ mesons, is extended to investigate the change of hadron properties in finite nuclei. Relativistic Hartree equations for spherical nuclei have been derived from a relativistic quark model of the structure of bound nucleons and mesons. Using this unified, self-consistent description of both infinite nuclear matter and finite nuclei, we investigate the properties of some closed-shell nuclei, and study the changes in the hadron masses of the non-strange vector mesons, the hyperons and the nucleon in those nuclei. We find a new, simple scaling relation for the changes of the hadron masses, which can be described in terms of the number of non-strange quarks in the hadron and the value of the scalar mean-field in a nucleus.

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