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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...
Autores principales: | , , |
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Lenguaje: | eng |
Publicado: |
1994
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Materias: | |
Acceso en línea: | https://dx.doi.org/10.1016/0370-2693(94)90210-0 http://cds.cern.ch/record/629451 |
_version_ | 1780900601662537728 |
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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. |
id | cern-629451 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 1994 |
record_format | invenio |
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 |
work_keys_str_mv | AT papadopoulosna modelsofelectroweakinteractionsinnoncommutativegeometryacomparison AT plassj modelsofelectroweakinteractionsinnoncommutativegeometryacomparison AT scheckf modelsofelectroweakinteractionsinnoncommutativegeometryacomparison |