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dc.contributor.authorGirotti, Horacio Oscarpt_BR
dc.contributor.authorGomes, Marcelopt_BR
dc.contributor.authorSilva, Adilson J. dapt_BR
dc.date.accessioned2016-05-10T02:07:09Zpt_BR
dc.date.issued1992pt_BR
dc.identifier.issn0370-2693pt_BR
dc.identifier.urihttp://hdl.handle.net/10183/140614pt_BR
dc.description.abstractThe effective nonrelativistic potential VT describing the fermion-fermion interaction in the Maxwell-Chern-Simons theory is derived to the lowest order in perturbation theory. As expected, VT is not invariant under parity and time-reversal transformations. The quantum dynamics generated by Vr becomes exactly solvable at the limits where either the Maxwell or the Chern- Simons terms disappear; in neither case electron-electron bound states show up. However, numerical calculations indicate that fermion-fermion bound states do exist in the general case.en
dc.format.mimetypeapplication/pdfpt_BR
dc.language.isoengpt_BR
dc.relation.ispartofPhysics letters. B. Amsterdam. Vol. 274, no. 3/4 (Jan. 1992), p. 357-362pt_BR
dc.rightsOpen Accessen
dc.subjectFisica de particulas elementares e campospt_BR
dc.subjectTeoria quantica de campospt_BR
dc.subjectTeoria de perturbacaopt_BR
dc.subjectTeoria quantica de campos relativisticospt_BR
dc.titleThe fermion-fermion effective potential in the maxwell-chern-simons theorypt_BR
dc.typeArtigo de periódicopt_BR
dc.identifier.nrb000056072pt_BR
dc.type.originEstrangeiropt_BR


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