The non-anticommutative supersymmetric Wess-Zumino model

We discuss the non-anticommutative (N=1/2) supersymmetric Wess-Zumino model in four dimensions. Firstly we introduce differential operators which implement the non-anticommutative supersymmetry algebra acting on the component fields and action. Then we perform the renormalisation of the model up to...

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Detalles Bibliográficos
Autores principales: Jack, I, Jones, D R T, Purdy, R
Lenguaje:eng
Publicado: 2008
Materias:
Particle Physics - Theory
Acceso en línea:https://dx.doi.org/10.1088/1126-6708/2009/02/019
http://cds.cern.ch/record/1118968
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author Jack, I
Jones, D R T
Purdy, R
author_facet Jack, I
Jones, D R T
Purdy, R
author_sort Jack, I
collection CERN
description We discuss the non-anticommutative (N=1/2) supersymmetric Wess-Zumino model in four dimensions. Firstly we introduce differential operators which implement the non-anticommutative supersymmetry algebra acting on the component fields and action. Then we perform the renormalisation of the model up to two-loop order, including the complete set of terms necessary for renormalisability. We determine the form such an action must take in order to be preserved under renormalisation and show that only two such forms are possible, in one of which the action reduces to the ordinary N=1 action upon eliminating the auxiliary fields.
id cern-1118968
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2008
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spelling cern-11189682019-09-30T06:29:59Zdoi:10.1088/1126-6708/2009/02/019http://cds.cern.ch/record/1118968engJack, IJones, D R TPurdy, RThe non-anticommutative supersymmetric Wess-Zumino modelParticle Physics - TheoryWe discuss the non-anticommutative (N=1/2) supersymmetric Wess-Zumino model in four dimensions. Firstly we introduce differential operators which implement the non-anticommutative supersymmetry algebra acting on the component fields and action. Then we perform the renormalisation of the model up to two-loop order, including the complete set of terms necessary for renormalisability. We determine the form such an action must take in order to be preserved under renormalisation and show that only two such forms are possible, in one of which the action reduces to the ordinary N=1 action upon eliminating the auxiliary fields.arXiv:0808.0400LTH799oai:cds.cern.ch:11189682008-08-05
spellingShingle Particle Physics - Theory
Jack, I
Jones, D R T
Purdy, R
The non-anticommutative supersymmetric Wess-Zumino model
title The non-anticommutative supersymmetric Wess-Zumino model
title_full The non-anticommutative supersymmetric Wess-Zumino model
title_fullStr The non-anticommutative supersymmetric Wess-Zumino model
title_full_unstemmed The non-anticommutative supersymmetric Wess-Zumino model
title_short The non-anticommutative supersymmetric Wess-Zumino model
title_sort non-anticommutative supersymmetric wess-zumino model
topic Particle Physics - Theory
url https://dx.doi.org/10.1088/1126-6708/2009/02/019
http://cds.cern.ch/record/1118968
work_keys_str_mv AT jacki thenonanticommutativesupersymmetricwesszuminomodel
AT jonesdrt thenonanticommutativesupersymmetricwesszuminomodel
AT purdyr thenonanticommutativesupersymmetricwesszuminomodel
AT jacki nonanticommutativesupersymmetricwesszuminomodel
AT jonesdrt nonanticommutativesupersymmetricwesszuminomodel
AT purdyr nonanticommutativesupersymmetricwesszuminomodel

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