Rotated Branes and N=1 Duality

We consider configurations of rotated NS-branes leading to a family of four-dimensional N=1 super-QCD theories, interpolating between four-dimensional analogues of the Hanany-Witten vacua, and the Elitzur-Giveon-Kutasov configuration for N=1 duality. The rotation angle is the N=2 breaking parameter,...

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Detalles Bibliográficos
Autor principal: Barbon, J.L.F.
Lenguaje:eng
Publicado: 1997
Materias:
Particle Physics - Theory
Acceso en línea:https://dx.doi.org/10.1016/S0370-2693(97)00451-6
http://cds.cern.ch/record/321901
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author Barbon, J.L.F.
author_facet Barbon, J.L.F.
author_sort Barbon, J.L.F.
collection CERN
description We consider configurations of rotated NS-branes leading to a family of four-dimensional N=1 super-QCD theories, interpolating between four-dimensional analogues of the Hanany-Witten vacua, and the Elitzur-Giveon-Kutasov configuration for N=1 duality. The rotation angle is the N=2 breaking parameter, the mass of the adjoint scalar in the N=2 vector multiplet. We add some comments on the relevance of these configurations as possible stringy proofs of N=1 duality.
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institution Organización Europea para la Investigación Nuclear
language eng
publishDate 1997
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spelling cern-3219012023-03-14T20:33:09Zdoi:10.1016/S0370-2693(97)00451-6http://cds.cern.ch/record/321901engBarbon, J.L.F.Rotated Branes and N=1 DualityParticle Physics - TheoryWe consider configurations of rotated NS-branes leading to a family of four-dimensional N=1 super-QCD theories, interpolating between four-dimensional analogues of the Hanany-Witten vacua, and the Elitzur-Giveon-Kutasov configuration for N=1 duality. The rotation angle is the N=2 breaking parameter, the mass of the adjoint scalar in the N=2 vector multiplet. We add some comments on the relevance of these configurations as possible stringy proofs of N=1 duality.We consider configurations of rotated NS-branes leading to a family of four-dimensional N=1 super-QCD theories, interpolating between four-dimensional analogues of the Hanany-Witten vacua, and the Elitzur-Giveon-Kutasov configuration for N=1 duality. The rotation angle is the N=2 breaking parameter, the mass of the adjoint scalar in the N=2 vector multiplet. We add some comments on the relevance of these configurations as possible stringy proofs of N=1 duality.We consider configurations of rotated NS -branes leading to a family of four-dimensional N = 1 super-QCD theories, interpolating between four-dimensional analogues of the Hanany-Witten vacua, and the Elitzur-Giveon-Kutasov configuration for N = 1 duality. The rotation angle is the N = 2 breaking parameter, the mass of the adjoint scalar in the N = 2 vector multiplet. We add some comments on the relevance of these configurations as possible stringy proofs of N = 1 duality.hep-th/9703051CERN-TH-97-038CERN-TH-97-38CERN-TH-97-038oai:cds.cern.ch:3219011997-03-06
spellingShingle Particle Physics - Theory
Barbon, J.L.F.
Rotated Branes and N=1 Duality
title Rotated Branes and N=1 Duality
title_full Rotated Branes and N=1 Duality
title_fullStr Rotated Branes and N=1 Duality
title_full_unstemmed Rotated Branes and N=1 Duality
title_short Rotated Branes and N=1 Duality
title_sort rotated branes and n=1 duality
topic Particle Physics - Theory
url https://dx.doi.org/10.1016/S0370-2693(97)00451-6
http://cds.cern.ch/record/321901
work_keys_str_mv AT barbonjlf rotatedbranesandn1duality

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