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dc.contributor.authorBodmann, Bardo Ernst Josefpt_BR
dc.contributor.authorMaris, Theodor August Johannespt_BR
dc.date.accessioned2016-05-14T02:08:26Zpt_BR
dc.date.issued2000pt_BR
dc.identifier.issn0370-2693pt_BR
dc.identifier.urihttp://hdl.handle.net/10183/141135pt_BR
dc.description.abstractThe present investigation is an attempt to understand the fermion mass ratios in the framework of QED of charged fermions without a bare mass. Since QED of massless charged fermions is invariant under the dilatation transformation, this symmetry has to be spontaneously broken to obtain massive fermions. In the proposed model we combine a mass-scale normalisation with the renormalisation procedure, assuming the fermion momentum space being a four-dimensional one-shell hyperboloid embedded in a five-dimensional space. The hyperboloid constrains the allowed fermion field solutions. We construct the theory in the conventional way using equal time anti-commutator and the Lagrangian formalism. Starting from the Dyson–Schwinger equation for fermion propagator in the Landau gauge, we derive the fermion mass function and self-reciprocal solutions for the mass ratios, which are independent of any constant.en
dc.format.mimetypeapplication/pdf
dc.language.isoengpt_BR
dc.relation.ispartofPhysics letters. B. Amsterdam. Vol. 495, no. 1/2 (Dec. 2000), p. 98-104pt_BR
dc.rightsOpen Accessen
dc.subjectCurved energy–momentum spaceen
dc.subjectFísicapt_BR
dc.subjectFermion mass ratiosen
dc.titleSelf-reciprocal fermion mass ratios from massless QED with curved momentum spacept_BR
dc.typeArtigo de periódicopt_BR
dc.identifier.nrb000291414pt_BR
dc.type.originEstrangeiropt_BR


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