Abstract

We develop an effective superpotential formalism for the SU(2)×U(1) invariant sector of mathcal{N} = 2 gauged supergravity in five dimensions with a U(1)3 Fayet-Iliopoulos gauging, and determine the exact superpotential that describes all 1/4 BPS solutions in this sector. This includes the Gutowski-Reall black holes, but also a much broader class of solutions with a squashed S3, magnetic flux and vector multiplet sources, as well as complex Euclidean BPS saddles. Some of these solutions are known only numerically, but the exact superpotential allows us to analytically evaluate the on-shell action, holographic one-point functions and conserved charges of all BPS solutions and to study their thermodynamics. In particular, by examining the supersymmetry Ward identities we show that solutions with supersymmetric vector multiplet sources break supersymmetry spontaneously. We also demonstrate the first law for black holes in the SU(2)×U(1) invariant sector and show that the conserved charges of supersymmetric solutions satisfy the generalized BPS relation derived in [1], which includes the supersymmetric Casimir energy as a consequence of the anomalous supersymmetry transformation of the mathcal{N} = 1 supercurrent at the boundary. Finally, we show that the effective superpotential provides a unifying entropy extremization principle, reproducing Sen’s entropy function for near extremal black holes and the Hosseini-Hristov-Zaffaroni functional for complex Euclidean BPS saddles.

Highlights

  • By examining the supersymmetry Ward identities we show that solutions with supersymmetric vector multiplet sources break supersymmetry spontaneously

  • We focus on the SU(2)×U(1) invariant sector and show that both the conserved charges and the on-shell action of generic black holes within this sector are determined by the effective superpotential

  • We present three exact effective superpotentials that describe respectively the general Reissner-Nordström-Anti de Sitter (AdS) black hole, the near horizon region of non-supersymmetric extremal black holes, and all SU(2)×U(1) invariant 1/4 BPS solutions

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Summary

Introduction and summary

JHEP03(2022) where the reduced superpotential, F , depends only on the difference, u, of the generalized coordinates u1 and u2 , and U0 is a constant This is a general result for all solutions with a non-compact timelike isometry, but we will verify it explicitly in the examples we will discuss later or, including all 1/4 BPS black holes. As we explain in appendix C, using the BPS superpotential in (3.65) in the flow equations (3.25), one can verify that the quantities (3.67) are constants of motion (4.112), as well as the constraint (4.119), while it gives the correct value for the entropy at the extremum

Discussion and future directions
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