On non-abelian T-dual geometries with Ramond fluxes
By K. Sfetsos, D. Thompson. 2010
235 citations recorded by the source corpus.
Abstract We show how to implement T-duality along non-abelian isometries in backgrounds with non-vanishing Ramond fields. When the dimension of the isometry group is odd (even) the duality swaps (preserves) the chirality of the theory. In certain cases a non-abelian duality can result in a massive type-IIA background. We provide two examples by dualising SU ( 2 ) isometry subgroups in AdS 5 × S 5 and AdS 3 × S 3 × T 4 . The resultant dual geometries inherit the original AdS factors but have transverse spaces with reduced isometry and preserve only half of the original supersymmetry. The non-abelian dual of AdS 5 × S 5 has an M-theory lift which is related to the gravity duals of N = 2 superconformal theories. We comment on a possible interpretation of this as a high spin limit.
Subfields: Astronomy and Astrophysics, Nuclear and High Energy Physics, Statistical and Nonlinear Physics
View Paper: https://www.semanticscholar.org/paper/4d519fa4ac0e579417235040aff0daa9f6c2aee9
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Citations in the corpus
- Integrable interpolations: From exact CFTs to non-Abelian T-duals (2013, methodology): “It was shown in [10] that when supported by appropriate flux fields it is a solution of massive IIA-supergravity and that it represent the non-Abelian T-dual of the background corresponding to the near horizon of the D1-D5 brane system.”
- Duality Symmetric String and M-Theory (2013, methodology): “Both of these generalisation have been studied in recent years and have led to some surprising insights especially within the context of the AdS/CFT correspondence; non-Abelian T-dualities have been used to generate interesting new supergravity backgrounds [30, 31, 32, 33, 34, 35, 36] and selfdualit”
- Non-Abelian T-duality and the AdS/CFT correspondence: New N=1 backgrounds (2013, methodology): “After non-abelian T-duality, the corresponding "UV" geometry will just be some Z2 quotient of the Gaiotto-Maldacena type geometry found in [10] and the "IR" geometry the result provide in the preceding section (the Klebanov-Witten transformed).”