Incompressibility of nuclear matter, and Coulomb and volume-symmetry coefficients of nucleus incompressibility in the relativistic mean field theory

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dc.creatorKouno, H.
dc.creatorMitsumori, T.
dc.creatorNoda, N.
dc.creatorKoide, K.
dc.creatorHasegawa, A.
dc.creatorNakano, M.
dc.date1995-07-10
dc.date.accessioned2026-07-07T11:15:24Z
dc.date.available2026-07-07T11:15:24Z
dc.descriptionThe volume coefficient $K$(=incompressibility of the nuclear matter), the Coulomb coefficient $K_c$, and the volume-symmetry coefficient $K_{vs}$ of the nucleus incompressibility are studied in the framework of the relativistic mean field theory, with aid of the scaling model. It is found that $K= 300\pm 50$MeV is necessary to account for the empirical values of $K_v$, $K_c$, and $K_{vs}$, simultaneously. The result is independent on the detail descriptions of the potential of the $σ$-meson self-interaction and is almost independent of the strength of the $ω$-meson self-interaction.
dc.descriptionPACS numbers: 21.65.+f, 21.30.+y
dc.identifierhttps://arxiv.org/abs/nucl-th/9507013
dc.identifierhttp://arxiv.org/abs/nucl-th/9507013
dc.identifierPhys.Rev.C53:2542-2545,1996
dc.identifierdoi:10.1103/PhysRevC.53.2542
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/192379
dc.subjectNuclear Theory
dc.titleIncompressibility of nuclear matter, and Coulomb and volume-symmetry coefficients of nucleus incompressibility in the relativistic mean field theory
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