Abstract Employing the method applied to construct AdS5 solutions from M5-branes recently by Bah, Bonetti, Minasian and Nardoni, we construct supersymmetric AdS3 solutions from D3-branes and M5-branes wrapped on a… Click to show full abstract
Abstract Employing the method applied to construct AdS5 solutions from M5-branes recently by Bah, Bonetti, Minasian and Nardoni, we construct supersymmetric AdS3 solutions from D3-branes and M5-branes wrapped on a disc with non-trivial holonomies at the boundary. In five-dimensional U(1)3-gauged $$ \mathcal{N} $$ N = 2 supergravity, we find $$ \mathcal{N} $$ N = (2, 2) and $$ \mathcal{N} $$ N = (4, 4) supersymmetric AdS3 solutions. We uplift the solutions to type IIB supergravity and obtain D3-branes wrapped on a topological disc. We also uplift the solutions to eleven-dimensional supergravity and obtain M5-branes wrapped on a product of topological disc and Riemann surface. For the $$ \mathcal{N} $$ N = (2, 2) solution, holographic central charges are finite and well-defined. On the other hand, we could not find $$ \mathcal{N} $$ N = (4, 4) solution with finite holographic central charge. Finally, we show that the topological disc we obtain is, in fact, identical to a special case of the multi-charge spindle solution.
               
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