We construct a family of multi-dyonically charged and rotating supersymmetric AdS$_2 imes Sigma$ solutions of $D=4$, $mathcal{N}=4$ gauged supergravity, where $Sigma$ is a sphere with two conical singularities known as a spindle. We argue that these arise as near horizon limits of extremal dyonically charged rotating and accelerating supersymmetric black holes in AdS$_4$, that we conjecture to exist. We demonstrate this in the non-rotating limit, constructing the accelerating black hole solutions and showing that the non-spinning spindle solutions arise as the near horizon limit of the supersymmetric and extremal sub-class of these black holes. From the near horizon solutions we compute the Bekenstein-Hawking entropy of the black holes as a function of the conserved charges, and show that this may equivalently be obtained by extremizing a simple entropy function. For appropriately quantized magnetic fluxes, the solutions uplift on $S^7$, or its ${cal N}=4$ orbifolds $S^7/Gamma$, to smooth supersymmetric solutions to $D=11$ supergravity, where the entropy is expected to count microstates of the theory on $N$ M2-branes wrapped on a spinning spindle, in the large $N$ limit.

Multi-charge accelerating black holes and spinning spindles

Matteo Inglese;Dario Martelli;
2022-01-01

Abstract

We construct a family of multi-dyonically charged and rotating supersymmetric AdS$_2 imes Sigma$ solutions of $D=4$, $mathcal{N}=4$ gauged supergravity, where $Sigma$ is a sphere with two conical singularities known as a spindle. We argue that these arise as near horizon limits of extremal dyonically charged rotating and accelerating supersymmetric black holes in AdS$_4$, that we conjecture to exist. We demonstrate this in the non-rotating limit, constructing the accelerating black hole solutions and showing that the non-spinning spindle solutions arise as the near horizon limit of the supersymmetric and extremal sub-class of these black holes. From the near horizon solutions we compute the Bekenstein-Hawking entropy of the black holes as a function of the conserved charges, and show that this may equivalently be obtained by extremizing a simple entropy function. For appropriately quantized magnetic fluxes, the solutions uplift on $S^7$, or its ${cal N}=4$ orbifolds $S^7/Gamma$, to smooth supersymmetric solutions to $D=11$ supergravity, where the entropy is expected to count microstates of the theory on $N$ M2-branes wrapped on a spinning spindle, in the large $N$ limit.
2022
105
12
126001
126024
http://arxiv.org/abs/2109.14625v3
High Energy Physics - Theory
Pietro Ferrero; Matteo Inglese; Dario Martelli; James Sparks
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/2318/1865650
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