Perturbation theory in a deformed basis

cnea.localizacion02.79.09
cnea.tipodocumentoPRESENTACIÓN A EVENTO
dc.contributor.authorBes, Daniel R.
dc.date.accessioned2024-02-09T15:35:42Z
dc.date.available2024-02-09T15:35:42Z
dc.date.issued1979
dc.description.abstractThe total Hamiltonian H is written in two parts H = H0 + x Hres ( 0 ≤ x ≤ 1 ). We consider the case in which the basic set of states (eigenfunctions of H0) is deformed, i.e., [H,L] = O and [H0,L] ≠ O, where L can be the angular momentum, the number of particles, etc. In such cases perturbation theory of Hres converge.
dc.description.institutionalaffiliationFil: Bes, Daniel R. Comisión Nacional de Energía Atómica; Argentina
dc.format.extent4 p.
dc.format.mediumapplication/pdf
dc.identifier.urihttps://nuclea.cnea.gob.ar/handle/20.500.12553/4682
dc.language.ISO639-3eng
dc.publisherComisión Nacional de Energía Atómica (Argentina)
dc.relation.ispartofProceedings of the Third Latin American Workshop on Selfconsistent Theories of Condensed Matter. Buenos Aires, July 2-13, 1979
dc.rights.accesslevelinfo:eu-repo/semantics/openAccess
dc.rights.urihttps://creativecommons.org/licenses/by-nc-sa/4.0/
dc.subject.keywordPERTURBATION THEORY
dc.subject.keywordTEORIA DE LAS PERTURBACIONES
dc.subject.keywordHAMILTONIAN FUNCTION
dc.subject.keywordFUNCION DE HAMILTON
dc.titlePerturbation theory in a deformed basis
dc.typePRESENTACIÓN A EVENTO
dc.type.openaireinfo:eurepo/semantics/conferenceObject
dc.type.snrdinfo:arrepo/semantics/documento de conferencia
dc.type.versioninfo:eu-repo/semantics/publishedVersion
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