Studies of the ABJM Theory in a Formulation with Manifest SU(4) R-Symmetry
We examine the three-dimensional N = 6 superconformal Chern--Simons theory with U(N) X U(N) gauge symmetry, which was recently constructed by Aharony, Bergman, Jafferis, and Maldacena (ABJM). Using a formulation with manifest SU(4) R-symmetry and no auxiliary fields, we verify in complete detail bot...
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Materyal Türü: | Journal article |
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2008
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author | Bandres, M Lipstein, A Schwarz, J |
author_facet | Bandres, M Lipstein, A Schwarz, J |
author_sort | Bandres, M |
collection | OXFORD |
description | We examine the three-dimensional N = 6 superconformal Chern--Simons theory with U(N) X U(N) gauge symmetry, which was recently constructed by Aharony, Bergman, Jafferis, and Maldacena (ABJM). Using a formulation with manifest SU(4) R-symmetry and no auxiliary fields, we verify in complete detail both the Poincare supersymmetry and the conformal supersymmetry of the action. Together, these imply the complete OSp(6|4) superconformal symmetry of the theory. The potential, which is sixth order in scalar fields, is recast as a sum of squares. |
first_indexed | 2024-03-07T01:50:19Z |
format | Journal article |
id | oxford-uuid:99ddc489-3b7c-494c-a9cf-3f420efdb4c5 |
institution | University of Oxford |
last_indexed | 2024-03-07T01:50:19Z |
publishDate | 2008 |
record_format | dspace |
spelling | oxford-uuid:99ddc489-3b7c-494c-a9cf-3f420efdb4c52022-03-27T00:17:21ZStudies of the ABJM Theory in a Formulation with Manifest SU(4) R-SymmetryJournal articlehttp://purl.org/coar/resource_type/c_dcae04bcuuid:99ddc489-3b7c-494c-a9cf-3f420efdb4c5Symplectic Elements at Oxford2008Bandres, MLipstein, ASchwarz, JWe examine the three-dimensional N = 6 superconformal Chern--Simons theory with U(N) X U(N) gauge symmetry, which was recently constructed by Aharony, Bergman, Jafferis, and Maldacena (ABJM). Using a formulation with manifest SU(4) R-symmetry and no auxiliary fields, we verify in complete detail both the Poincare supersymmetry and the conformal supersymmetry of the action. Together, these imply the complete OSp(6|4) superconformal symmetry of the theory. The potential, which is sixth order in scalar fields, is recast as a sum of squares. |
spellingShingle | Bandres, M Lipstein, A Schwarz, J Studies of the ABJM Theory in a Formulation with Manifest SU(4) R-Symmetry |
title | Studies of the ABJM Theory in a Formulation with Manifest SU(4)
R-Symmetry |
title_full | Studies of the ABJM Theory in a Formulation with Manifest SU(4)
R-Symmetry |
title_fullStr | Studies of the ABJM Theory in a Formulation with Manifest SU(4)
R-Symmetry |
title_full_unstemmed | Studies of the ABJM Theory in a Formulation with Manifest SU(4)
R-Symmetry |
title_short | Studies of the ABJM Theory in a Formulation with Manifest SU(4)
R-Symmetry |
title_sort | studies of the abjm theory in a formulation with manifest su 4 r symmetry |
work_keys_str_mv | AT bandresm studiesoftheabjmtheoryinaformulationwithmanifestsu4rsymmetry AT lipsteina studiesoftheabjmtheoryinaformulationwithmanifestsu4rsymmetry AT schwarzj studiesoftheabjmtheoryinaformulationwithmanifestsu4rsymmetry |