Five-Dimensional Gauged Supergravity and Supersymmetry Breaking in $M$ Theory

We extend the formulation of gauged supergravity in five dimensions, as obtained by compactification of $M$~theory on a deformed Calabi-Yau manifold, to include non-universal matter hypermultiplets. Even in the presence of this gauging, only the graviton supermultiplets and matter hypermultiplets ca...

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Detalles Bibliográficos
Autores principales: Ellis, John R., Lalak, Zygmunt, Pokorski, Witold
Lenguaje:eng
Publicado: 1998
Materias:
Particle Physics - Theory
Acceso en línea:https://dx.doi.org/10.1016/S0550-3213(99)00469-1
http://cds.cern.ch/record/371223
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author Ellis, John R.
Lalak, Zygmunt
Pokorski, Witold
author_facet Ellis, John R.
Lalak, Zygmunt
Pokorski, Witold
author_sort Ellis, John R.
collection CERN
description We extend the formulation of gauged supergravity in five dimensions, as obtained by compactification of $M$~theory on a deformed Calabi-Yau manifold, to include non-universal matter hypermultiplets. Even in the presence of this gauging, only the graviton supermultiplets and matter hypermultiplets can couple to supersymmetry breaking sources on the walls, though these mix with vector supermultiplets in the bulk. Whatever the source of supersymmetry breaking on the hidden wall, that on the observable wall is in general a combination of dilaton- and moduli-dominated scenarios.
id cern-371223
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 1998
record_format invenio
spelling cern-3712232023-03-14T20:09:31Zdoi:10.1016/S0550-3213(99)00469-1http://cds.cern.ch/record/371223engEllis, John R.Lalak, ZygmuntPokorski, WitoldFive-Dimensional Gauged Supergravity and Supersymmetry Breaking in $M$ TheoryParticle Physics - TheoryWe extend the formulation of gauged supergravity in five dimensions, as obtained by compactification of $M$~theory on a deformed Calabi-Yau manifold, to include non-universal matter hypermultiplets. Even in the presence of this gauging, only the graviton supermultiplets and matter hypermultiplets can couple to supersymmetry breaking sources on the walls, though these mix with vector supermultiplets in the bulk. Whatever the source of supersymmetry breaking on the hidden wall, that on the observable wall is in general a combination of dilaton- and moduli-dominated scenarios.We extend the formulation of gauged supergravity in five dimensions, as obtained by compactification of $M$~theory on a deformed Calabi-Yau manifold, to include non-universal matter hypermultiplets. Even in the presence of this gauging, only the graviton supermultiplets and matter hypermultiplets can couple to supersymmetry breaking sources on the walls, though these mix with vector supermultiplets in the bulk. Whatever the source of supersymmetry breaking on the hidden wall, that on the observable wall is in general a combination of dilaton- and moduli-dominated scenarios.We extend the formulation of gauged supergravity in five dimensions, as obtained by compactification of $M$~theory on a deformed Calabi-Yau manifold, to include non-universal matter hypermultiplets. Even in the presence of this gauging, only the graviton supermultiplets and matter hypermultiplets can couple to supersymmetry breaking sources on the walls, though these mix with vector supermultiplets in the bulk. Whatever the source of supersymmetry breaking on the hidden wall, that on the observable wall is in general a combination of dilaton- and moduli-dominated scenarios.We extend the formulation of gauged supergravity in five dimensions, as obtained by compactification of $M$~theory on a deformed Calabi-Yau manifold, to include non-universal matter hypermultiplets. Even in the presence of this gauging, only the graviton supermultiplets and matter hypermultiplets can couple to supersymmetry breaking sources on the walls, though these mix with vector supermultiplets in the bulk. Whatever the source of supersymmetry breaking on the hidden wall, that on the observable wall is in general a combination of dilaton- and moduli-dominated scenarios.We extend the formulation of gauged supergravity in five dimensions, as obtained by compactification of M-theory on a deformed Calabi-Yau manifold, to include non-universal matter hypermultiplets. Even in the presence of this gauging, only the graviton supermultiplet and matter hypermultiplets can couple to supersymmetry breaking sources on the walls, though these mix with vector supermultiplets in the bulk. Whatever the source of supersymmetry breaking on the hidden wall, that on the observable wall is in general a combination of dilaton- and moduli-dominated scenarios.hep-th/9811133CERN-TH-98-359OUTP-98-77-PCERN-TH-98-359OUTP-98-77-Poai:cds.cern.ch:3712231998-11-16
spellingShingle Particle Physics - Theory
Ellis, John R.
Lalak, Zygmunt
Pokorski, Witold
Five-Dimensional Gauged Supergravity and Supersymmetry Breaking in $M$ Theory
title Five-Dimensional Gauged Supergravity and Supersymmetry Breaking in $M$ Theory
title_full Five-Dimensional Gauged Supergravity and Supersymmetry Breaking in $M$ Theory
title_fullStr Five-Dimensional Gauged Supergravity and Supersymmetry Breaking in $M$ Theory
title_full_unstemmed Five-Dimensional Gauged Supergravity and Supersymmetry Breaking in $M$ Theory
title_short Five-Dimensional Gauged Supergravity and Supersymmetry Breaking in $M$ Theory
title_sort five-dimensional gauged supergravity and supersymmetry breaking in $m$ theory
topic Particle Physics - Theory
url https://dx.doi.org/10.1016/S0550-3213(99)00469-1
http://cds.cern.ch/record/371223
work_keys_str_mv AT ellisjohnr fivedimensionalgaugedsupergravityandsupersymmetrybreakinginmtheory
AT lalakzygmunt fivedimensionalgaugedsupergravityandsupersymmetrybreakinginmtheory
AT pokorskiwitold fivedimensionalgaugedsupergravityandsupersymmetrybreakinginmtheory

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