Large AdS black holes from QFT

Choi, Sunjin; Kim, Joon-Ho; Kim, Seok; Nahmgoong, June

doi:10.48550/arxiv.1810.12067

Cited by 103 publications

(403 citation statements)

References 51 publications

(176 reference statements)

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“…Similar results were obtained in [10,11]. These developments built upon the original counting for rotating, electrically charged, asymptotically AdS 5 black holes via the superconformal index of N " 4 maximally supersymmetric Yang-Mills [12][13][14] which has also been extended to black holes in AdS 6 [15] and AdS 7 [16,17]. These impressive results set the stage for precision entropy counting and we hope that this manuscript will serve as a handbook for computations on the gravitational side.…”

supporting

confidence: 67%

Non-topological logarithmic corrections in minimal gauged supergravity

David,

Godet,

Liu

et al. 2021

Preprint

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We compute the logarithmic correction to the entropy of asymptotically AdS 4 black holes in minimal N " 2 gauged supergravity. We show that for extremal black holes the logarithmic correction computed in the near horizon geometry agrees with the result in the full geometry up to zero mode contributions, thus clarifying where the quantum degrees of freedom lie in AdS spacetimes. In contrast to flat space, we observe that the logarithmic correction for supersymmetric black holes can be non-topological in AdS as it is controlled by additional four-derivative terms other than the Euler density. The available microscopic data and results in 11d supergravity indicate that the full logarithmic correction is topological, which suggests that the topological nature of logarithmic corrections could serve as a diagnosis of whether a low-energy gravity theory admits an ultraviolet completion.

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confidence: 67%

Non-topological logarithmic corrections in minimal gauged supergravity

David,

Godet,

Liu

et al. 2021

Preprint

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“…There has been recently a lot of progress in the microscopic derivation of the entropy of anti de Sitter (AdS) black holes, starting with the magnetically charged and topologically twisted ones in AdS 4 × S 7 [1] and followed by the Kerr-Newman (KN) black holes in AdS 5 ×S 5 [2][3][4]. This analysis has been extended to many other black objects in AdS d , with d = 4, 5, 6, 7 with different types of electromagnetic charges and rotations and with various amounts of supersymmetry.…”

Section: Introductionmentioning

confidence: 99%

The joy of factorization at large $N$: five-dimensional indices and AdS black holes

Hosseini,

Yaakov,

Zaffaroni

2021

Preprint

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We discuss the large N factorization properties of five-dimensional supersymmetric partition functions for CFT with a holographic dual. We consider partition functions on manifolds of the form M = M 3 × S 2 , where is an equivariant parameter for rotation. We show that, when M 3 is a squashed three-sphere, the large N partition functions can be obtained by gluing elementary blocks associated with simple physical quantities. The same is true for various observables of the theories on M 3 = Σ g × S 1 , where Σ g is a Riemann surface of genus g, and, with a natural assumption on the form of the saddle point, also for the partition function, corresponding to either the topologically twisted index or a mixed one. This generalizes results in three and four dimensions and correctly reproduces the entropy of known black objects in AdS 6 × w S 4 and AdS 7 × S 4 . We also provide the supersymmetric background and explicitly perform localization for the mixed index on Σ g × S 1 × S 2 , filling a gap in the literature.

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“…We also note that some of the large N techniques explored in this paper might find applications to study black holes in AdS 4 /CFT 3 , AdS 6 /CFT 5 or AdS 7 /CFT 6 . These problems have been studied in [38,39,40], [41,42] and [11,43,44], but we think we can do more interesting…”

Section: Discussionmentioning

confidence: 99%

“…After extremizing this function with δ I , σ, τ subject to the constraint I δ I − σ − τ = −1, one takes the real part Re(S) to get the entropy [11,28,13]. This computation can be done easily using the universal form (4.12), by noting that primed variables δ ′ I , σ ′ , τ ′ are K times δ I , σ, τ apart from real constant shifts.…”

Section: Multi-cut Saddle Pointsmentioning

confidence: 99%

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Exact QFT duals of AdS black holes

Choi¹,

Jeong²,

Kim³

et al. 2021

Preprint

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We construct large N saddle points of the matrix model for the N = 4 Yang-Mills index dual to the BPS black holes in AdS 5 × S 5 , in two different setups. When the two complex chemical potentials for the angular momenta are collinear, we find linear eigenvalue distributions which solve the large N saddle point equation. When the chemical potentials are not collinear, we find novel solutions given by areal eigenvalue distributions after slightly reformulating the saddle point problem. We also construct a class of multicut saddle points, showing that they sometimes admit nontrivial filling fractions. As a byproduct, we find that the Bethe ansatz equation emerges from our saddle point equation.

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Large AdS black holes from QFT

Cited by 103 publications

References 51 publications

Non-topological logarithmic corrections in minimal gauged supergravity

Non-topological logarithmic corrections in minimal gauged supergravity

The joy of factorization at large $N$: five-dimensional indices and AdS black holes

Exact QFT duals of AdS black holes

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