Effective nucleon mass in relativistic mean field theory
| dc.creator | Chung, K. C. | |
| dc.creator | Wang, C. S. | |
| dc.creator | Santiago, A. J. | |
| dc.creator | Zhang, J. W. | |
| dc.date | 2001-02-01 | |
| dc.date.accessioned | 2026-07-07T05:38:26Z | |
| dc.date.available | 2026-07-07T05:38:26Z | |
| dc.description | In the $σ$-$ω$-$ρ$ model of the relativistic mean field theory with nonlinear $σ$-meson self-interaction, the effective nucleon mass $M^*$ is discussed with relation to the symmetry incompressibility $K_s$ of nuclear matter, based on the model parameters fitted to nuclear matter properties. It is shown that $M^*$ is larger than $0.73M$, if $K_s$ is assumed to be negative and the nuclear matter incompressibility $K_0$ is kept less than $300 MeV$. Furthermore, the field system is shown to be stable, as the $σ$-meson self-interaction energy is lower bounded in this parameter region. | |
| dc.description | 5 pages, 8 figures | |
| dc.identifier | https://arxiv.org/abs/nucl-th/0102001 | |
| dc.identifier | http://arxiv.org/abs/nucl-th/0102001 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/81612 | |
| dc.subject | Nuclear Theory | |
| dc.title | Effective nucleon mass in relativistic mean field theory | |
| dc.type | text |