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Please use this identifier to cite or link to this item: http://acervodigital.unesp.br/handle/11449/65815
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dc.contributor.authorCoutinho, F. A B-
dc.contributor.authorNogami, Y.-
dc.contributor.authorTomio, Lauro-
dc.date.accessioned2014-05-27T11:19:45Z-
dc.date.accessioned2016-10-25T18:15:47Z-
dc.date.available2014-05-27T11:19:45Z-
dc.date.available2016-10-25T18:15:47Z-
dc.date.issued1999-08-01-
dc.identifierhttp://dx.doi.org/10.1119/1.19362-
dc.identifier.citationAmerican Journal of Physics, v. 67, n. 8, p. 735-736, 1999.-
dc.identifier.issn0002-9505-
dc.identifier.urihttp://hdl.handle.net/11449/65815-
dc.identifier.urihttp://acervodigital.unesp.br/handle/11449/65815-
dc.description.abstractFor the electric polarizability of a bound system in relativistic quantum theory, there are two definitions that have appeared in the literature. They differ depending on whether or not the vacuum background is included in the system. A recent confusion in this connection is clarified. © 1999 American Associations of Physics Teachers.en
dc.format.extent735-736-
dc.language.isoeng-
dc.sourceScopus-
dc.titleTwo definitions of the electric polarizability of a bound system in relativistic quantum theoryen
dc.typeoutro-
dc.contributor.institutionUniversidade de São Paulo (USP)-
dc.contributor.institutionMcMaster University-
dc.contributor.institutionUniversidade Estadual Paulista (UNESP)-
dc.description.affiliationFaculdade de Medicina Universidade de São Paulo, 01246-903 São Paulo-
dc.description.affiliationDepartment of Physics and Astronomy McMaster University, Hamilton, Ont. L8S 4M1-
dc.description.affiliationInst. de Fis. Teórica Universidade Estadual Paulista, 01405-900 São Paulo-
dc.description.affiliationUnespInst. de Fis. Teórica Universidade Estadual Paulista, 01405-900 São Paulo-
dc.identifier.doi10.1119/1.19362-
dc.identifier.wosWOS:000081597500017-
dc.rights.accessRightsAcesso restrito-
dc.identifier.file2-s2.0-0033412282.pdf-
dc.relation.ispartofAmerican Journal of Physics-
dc.identifier.scopus2-s2.0-0033412282-
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