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Anomalous U(1)s in Type I superstring vacua

We perform a systematic string computation of the masses of anomalous U(1) gauge bosons in four-dimensional orientifold vacua, and we study their localization properties in the internal (compactified) space. We find that N=1 supersymmetric sectors yield four-dimensional contributions, localized in t...

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Detalles Bibliográficos
Autores principales: Antoniadis, Ignatios, Kiritsis, Elias, Rizos, John
Lenguaje:eng
Publicado: 2002
Materias:
Acceso en línea:https://dx.doi.org/10.1016/S0550-3213(02)00458-3
http://cds.cern.ch/record/547710
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author Antoniadis, Ignatios
Kiritsis, Elias
Rizos, John
author_facet Antoniadis, Ignatios
Kiritsis, Elias
Rizos, John
author_sort Antoniadis, Ignatios
collection CERN
description We perform a systematic string computation of the masses of anomalous U(1) gauge bosons in four-dimensional orientifold vacua, and we study their localization properties in the internal (compactified) space. We find that N=1 supersymmetric sectors yield four-dimensional contributions, localized in the whole six-dimensional internal space, while N=2 sectors give contributions localized in four internal dimensions. As a result, the U(1) gauge fields can be much lighter than the string scale, so that when the latter is at the TeV, they can mediate new non-universal repulsive forces at submillimeter distances much stronger than gravity. We also point out that even U(1)s which are free of four-dimensional anomalies may acquire non-zero masses as a consequence of six-dimensional anomalies.
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institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2002
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spelling cern-5477102023-03-14T20:19:29Zdoi:10.1016/S0550-3213(02)00458-3http://cds.cern.ch/record/547710engAntoniadis, IgnatiosKiritsis, EliasRizos, JohnAnomalous U(1)s in Type I superstring vacuaParticle Physics - TheoryWe perform a systematic string computation of the masses of anomalous U(1) gauge bosons in four-dimensional orientifold vacua, and we study their localization properties in the internal (compactified) space. We find that N=1 supersymmetric sectors yield four-dimensional contributions, localized in the whole six-dimensional internal space, while N=2 sectors give contributions localized in four internal dimensions. As a result, the U(1) gauge fields can be much lighter than the string scale, so that when the latter is at the TeV, they can mediate new non-universal repulsive forces at submillimeter distances much stronger than gravity. We also point out that even U(1)s which are free of four-dimensional anomalies may acquire non-zero masses as a consequence of six-dimensional anomalies.We perform a systematic string computation of the masses of anomalous U(1) gauge bosons in four-dimensional orientifold vacua, and we study their localization properties in the internal (compactified) space. We find that N=1 supersymmetric sectors yield four-dimensional contributions, localized in the whole six-dimensional internal space, while N=2 sectors give contributions localized in four internal dimensions. As a result, the U(1) gauge fields can be much lighter than the string scale, so that when the latter is at the TeV, they can mediate new non-universal repulsive forces at submillimeter distances much stronger than gravity. We also point out that even U(1)s which are free of four-dimensional anomalies may acquire non-zero masses as a consequence of six-dimensional anomalies.We perform a systematic string computation of the masses of anomalous U (1) gauge bosons in four-dimensional orientifold vacua, and we study their localization properties in the internal (compactified) space. We find that N =1 supersymmetric sectors yield four-dimensional contributions, localized in the whole six-dimensional internal space, while N =2 sectors give contributions localized in four internal dimensions. As a result, the U (1) gauge fields can be much lighter than the string scale, so that when the latter is at the TeV, they can mediate new non-universal repulsive forces at submillimeter distances much stronger than gravity. We also point out that even U (1)'s which are free of four-dimensional anomalies may acquire non-zero masses as a consequence of six-dimensional anomalies.hep-th/0204153CERN-TH-2002-083LPTENS-02-21CERN-TH-2002-083LPT-ENS-2002-21oai:cds.cern.ch:5477102002-04-18
spellingShingle Particle Physics - Theory
Antoniadis, Ignatios
Kiritsis, Elias
Rizos, John
Anomalous U(1)s in Type I superstring vacua
title Anomalous U(1)s in Type I superstring vacua
title_full Anomalous U(1)s in Type I superstring vacua
title_fullStr Anomalous U(1)s in Type I superstring vacua
title_full_unstemmed Anomalous U(1)s in Type I superstring vacua
title_short Anomalous U(1)s in Type I superstring vacua
title_sort anomalous u(1)s in type i superstring vacua
topic Particle Physics - Theory
url https://dx.doi.org/10.1016/S0550-3213(02)00458-3
http://cds.cern.ch/record/547710
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AT kiritsiselias anomalousu1sintypeisuperstringvacua
AT rizosjohn anomalousu1sintypeisuperstringvacua