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The coupling of valence shell and particle-hole degrees of freedom in a partial random phase approximation

dc.contributor.authorRowe, D. J.en_US
dc.contributor.authorRochford, P.en_US
dc.contributor.authorLe Blanc, R.en_US
dc.date.accessioned2006-04-07T19:55:53Z
dc.date.available2006-04-07T19:55:53Z
dc.date.issued1987-03-02en_US
dc.identifier.citationRowe, D. J., Rochford, P., Le Blanc, R. (1987/03/02)."The coupling of valence shell and particle-hole degrees of freedom in a partial random phase approximation." Nuclear Physics A 464(1): 39-60. <http://hdl.handle.net/2027.42/26774>en_US
dc.identifier.urihttp://www.sciencedirect.com/science/article/B6TVB-47317SR-3N/2/c8cfb18313f05b3e3af055927e22cdf4en_US
dc.identifier.urihttps://hdl.handle.net/2027.42/26774
dc.description.abstractIt is well known that the random phase approximation breaks down in the absence of a substantial energy gap between occupied and unoccupied single-particle states. Particle-hole excitations are then inevitably accompanied by substantial rearrangements of the particles in the neighbourhood of the Fermi surface. To accommodate this situation, a partial RPA is introduced which corresponds to replacing only the particle-hole degrees of freedom by bosons but leaving the valence space degrees of freedom intact. The PRPA is therefore a mapping of the many-fermion dynamics into the dynamics of a coupled boson-valence space. In application of the PRPA, algebraic methods, of either a fermionic or Lie algebra type, can be introduced, if desired, to facilitate the treatment of the valence space degrees of freedom. Results of applications are presented in which the valence space particles are treated in the rotational and SU(3) models, and are coupled strongly to giant dipole and quadrupole resonances.en_US
dc.format.extent1430845 bytes
dc.format.extent3118 bytes
dc.format.mimetypeapplication/pdf
dc.format.mimetypetext/plain
dc.language.isoen_US
dc.publisherElsevieren_US
dc.titleThe coupling of valence shell and particle-hole degrees of freedom in a partial random phase approximationen_US
dc.typeArticleen_US
dc.rights.robotsIndexNoFollowen_US
dc.subject.hlbsecondlevelPhysicsen_US
dc.subject.hlbsecondlevelNuclear Engineering and Radiological Sciencesen_US
dc.subject.hlbtoplevelScienceen_US
dc.subject.hlbtoplevelEngineeringen_US
dc.description.peerreviewedPeer Revieweden_US
dc.contributor.affiliationumPhysics Department, The University of Michigan, Ann Arbor, Michigan, 48109, USAen_US
dc.contributor.affiliationotherDepartment of Physics, University of Toronto, Toronto, Ontario, M5S 1A7, Canadaen_US
dc.contributor.affiliationotherDepartment of Physics, University of Toronto, Toronto, Ontario, M5S 1A7, Canadaen_US
dc.description.bitstreamurlhttp://deepblue.lib.umich.edu/bitstream/2027.42/26774/1/0000326.pdfen_US
dc.identifier.doihttp://dx.doi.org/10.1016/0375-9474(87)90421-0en_US
dc.identifier.sourceNuclear Physics Aen_US
dc.owningcollnameInterdisciplinary and Peer-Reviewed


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