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Please use this identifier to cite or link to this item: http://acervodigital.unesp.br/handle/11449/32102
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dc.contributor.authorDey, J.-
dc.contributor.authorTomio, L.-
dc.contributor.authorDey, M.-
dc.contributor.authorFrederico, T.-
dc.date.accessioned2014-05-20T15:20:54Z-
dc.date.accessioned2016-10-25T17:54:06Z-
dc.date.available2014-05-20T15:20:54Z-
dc.date.available2016-10-25T17:54:06Z-
dc.date.issued1991-11-01-
dc.identifierhttp://dx.doi.org/10.1103/PhysRevC.44.2181-
dc.identifier.citationPhysical Review C. College Pk: American Physical Soc, v. 44, n. 5, p. 2181-2186, 1991.-
dc.identifier.issn0556-2813-
dc.identifier.urihttp://hdl.handle.net/11449/32102-
dc.identifier.urihttp://acervodigital.unesp.br/handle/11449/32102-
dc.description.abstract1/N(c) expansion in QCD (with N(c) the number of colors) suggests using a potential from meson sector (e.g., Richardson) for baryons. For light quarks a sigma-field has to be introduced to ensure chiral symmetry breaking (chi-SB). It is found that nuclear matter properties can be used to pin down the chi-SB modeling. All masses, M(N), m-sigma, m-omega, are found to scale with density. The equations are solved self-consistently.en
dc.format.extent2181-2186-
dc.language.isoeng-
dc.publisherAmerican Physical Soc-
dc.sourceWeb of Science-
dc.titleQUARK MEAN-FIELD THEORY AND CONSISTENCY WITH NUCLEAR-MATTERen
dc.typeoutro-
dc.contributor.institutionMAULANA AZAD COLL-
dc.contributor.institutionUniversity of Washington-
dc.contributor.institutionUniversidade Estadual Paulista (UNESP)-
dc.description.affiliationMAULANA AZAD COLL,DEPT PHYS,CALCUTTA 700013,INDIA-
dc.description.affiliationUNIV WASHINGTON,DEPT PHYS,INST NUCL THEORY,FM-15,SEATTLE,WA 98195-
dc.identifier.doi10.1103/PhysRevC.44.2181-
dc.identifier.wosWOS:A1991GP73500047-
dc.rights.accessRightsAcesso restrito-
dc.identifier.fileWOSA1991GP73500047.pdf-
dc.relation.ispartofPhysical Review C-
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