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Models of electroweak interactions in non-commutative geometry: a comparison

Alain Connes' construction of the standard model is based on a generalized Dirac-Yukawa operator and the K-cycle $(\HD ,D)$, with $\HD$ a fermionic Hilbert space. If this construction is reformulated at the level of the differential algebra then a direct comparison with the alternative approach...

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Detalles Bibliográficos
Autores principales: Papadopoulos, N.A., Plass, J., Scheck, F.
Lenguaje:eng
Publicado: 1994
Materias:
Acceso en línea:https://dx.doi.org/10.1016/0370-2693(94)90210-0
http://cds.cern.ch/record/629451
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author Papadopoulos, N.A.
Plass, J.
Scheck, F.
author_facet Papadopoulos, N.A.
Plass, J.
Scheck, F.
author_sort Papadopoulos, N.A.
collection CERN
description Alain Connes' construction of the standard model is based on a generalized Dirac-Yukawa operator and the K-cycle $(\HD ,D)$, with $\HD$ a fermionic Hilbert space. If this construction is reformulated at the level of the differential algebra then a direct comparison with the alternative approach by the Marseille-Mainz group becomes possible. We do this for the case of the toy model based on the structure group $U(1)\times U(1)$ and for the $SU(2)\times U(1)$ of electroweak interactions. Connes' results are recovered without the somewhat disturbing $\gamma_{5}$-factors in the fermion mass terms and Yukawa couplings. We discuss both constructions in the same framework and, in particular, pinpoint the origin of the difference in the Higgs potential obtained by them.
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institution Organización Europea para la Investigación Nuclear
language eng
publishDate 1994
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spelling cern-6294512023-03-14T19:27:28Zdoi:10.1016/0370-2693(94)90210-0http://cds.cern.ch/record/629451engPapadopoulos, N.A.Plass, J.Scheck, F.Models of electroweak interactions in non-commutative geometry: a comparisonParticle Physics - TheoryAlain Connes' construction of the standard model is based on a generalized Dirac-Yukawa operator and the K-cycle $(\HD ,D)$, with $\HD$ a fermionic Hilbert space. If this construction is reformulated at the level of the differential algebra then a direct comparison with the alternative approach by the Marseille-Mainz group becomes possible. We do this for the case of the toy model based on the structure group $U(1)\times U(1)$ and for the $SU(2)\times U(1)$ of electroweak interactions. Connes' results are recovered without the somewhat disturbing $\gamma_{5}$-factors in the fermion mass terms and Yukawa couplings. We discuss both constructions in the same framework and, in particular, pinpoint the origin of the difference in the Higgs potential obtained by them.Alain Connes' construction of the standard model is based on a generalized Dirac-Yukawa operator and the K-cycle $(\HD ,D)$, with $\HD$ a fermionic Hilbert space. If this construction is reformulated at the level of the differential algebra then a direct comparison with the alternative approach by the Marseille-Mainz group becomes possible. We do this for the case of the toy model based on the structure group $U(1)\times U(1)$ and for the $SU(2)\times U(1)$ of electroweak interactions. Connes' results are recovered without the somewhat disturbing $\gamma_{5}$-factors in the fermion mass terms and Yukawa couplings. We discuss both constructions in the same framework and, in particular, pinpoint the origin of the difference in the Higgs potential obtained by them.Alain Connes' construction of the standard model is based on a generalized Dirac-Yukawa operator and the K-cycle ( , D) , with a fermionic Hilbert space. If this construction is reformulated at the level of the differential algebra then a direct comparison with the alternative approach by the Marseille-Mainz group becomes possible. We do this for the case of the toy model based on the structure group U (1) × U (1) and for the SU (2) × U (1) of the electroweak interactions. Connes' and Lott's results are recovered without the somewhat disturbing γ 5 - factors in the fermion mass terms and Yukawa couplings. We discuss both constructions in the same framework and, in particular, pinpoint the origin of the difference in the Higgs potential obtained by them.hep-th/9401136MZ-TH-93-26MZ-TH-93-26oai:cds.cern.ch:6294511994
spellingShingle Particle Physics - Theory
Papadopoulos, N.A.
Plass, J.
Scheck, F.
Models of electroweak interactions in non-commutative geometry: a comparison
title Models of electroweak interactions in non-commutative geometry: a comparison
title_full Models of electroweak interactions in non-commutative geometry: a comparison
title_fullStr Models of electroweak interactions in non-commutative geometry: a comparison
title_full_unstemmed Models of electroweak interactions in non-commutative geometry: a comparison
title_short Models of electroweak interactions in non-commutative geometry: a comparison
title_sort models of electroweak interactions in non-commutative geometry: a comparison
topic Particle Physics - Theory
url https://dx.doi.org/10.1016/0370-2693(94)90210-0
http://cds.cern.ch/record/629451
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AT plassj modelsofelectroweakinteractionsinnoncommutativegeometryacomparison
AT scheckf modelsofelectroweakinteractionsinnoncommutativegeometryacomparison