A chiral symmetric relativistic mean field model with logarithmic sigma potential

dc.creatorTsubakihara, Kohsuke
dc.creatorOhnishi, Akira
dc.date2006-07-21
dc.date.accessioned2026-07-07T11:07:32Z
dc.date.available2026-07-07T11:07:32Z
dc.descriptionWe develop a chiral symmetric relativistic mean field model with logarithmic sigma potential derived in the strong coupling limit of the lattice QCD. We find that both of the nuclear matter and finite nuclei are well described in the present model. The normal vacuum is found to have global stability at zero and finite baryon densities, and an equation of state with moderate stiffness (K ~ 280 MeV) is obtained. The binding energies and charge radii of Z closed even-even nuclei are well reproduced in a wide mass range from C to Pb isotopes, except for the underestimates of binding energies in several jj closed nuclei.
dc.description19 pages, 6 figures
dc.identifierhttps://arxiv.org/abs/nucl-th/0607046
dc.identifierhttp://arxiv.org/abs/nucl-th/0607046
dc.identifierProg.Theor.Phys.117:903-921,2007
dc.identifierdoi:10.1143/PTP.117.903
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/189875
dc.subjectNuclear Theory
dc.titleA chiral symmetric relativistic mean field model with logarithmic sigma potential
dc.typetext

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