3d gravity as a random ensemble

A bstract We give further evidence that the matrix-tensor model studied in [1] is dual to AdS 3 gravity including the sum over topologies. This provides a 3D version of the duality between JT gravity and an ensemble of random Hamiltonians, in which the matrix and tensor provide random CFT 2 data subject to a potential that incorporates the bootstrap constraints. We show how the Feynman rules of the ensemble produce a sum over all 3-manifolds and how surgery is implemented by the matrix integral. The partition functions of the resulting 3d gravity theory agree with Virasoro TQFT (VTQFT) on a fixed, hyperbolic manifold. However, on non-hyperbolic geometries, our 3d gravity theory differs from VTQFT, leading to a difference in the eigenvalue statistics of the associated ensemble. As explained in [1], the Schwinger-Dyson (SD) equations of the matrix-tensor integral play a crucial role in understanding how gravity emerges in the limit that the ensemble localizes to exact CFT’s. We show how the SD equations can be translated into a combinatorial problem about 3-manifolds.

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Publication Details

Journal
Journal of High Energy Physics
Published
2025-02-28
DOI
https://doi.org/10.1007/jhep02(2025)208
Citations
10
Primary Topic
Black Holes and Theoretical Physics
Type
article
Field-Weighted Citation Impact
18.70

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article

3d gravity as a random ensemble

Daniel L. Jafferis, Gabriel Wong, Liza Rozenberg
10 citations
Journal of High Energy Physics
Black Holes and Theoretical Physics
18.70
article

3d gravity as a random ensemble

Daniel L. Jafferis, Gabriel Wong, Liza Rozenberg
article en
10 citations

Abstract

A bstract We give further evidence that the matrix-tensor model studied in [1] is dual to AdS 3 gravity including the sum over topologies. This provides a 3D version of the duality between JT gravity and an ensemble of random Hamiltonians, in which the matrix and tensor provide random CFT 2 data subject to a potential that incorporates the bootstrap constraints. We show how the Feynman rules of the ensemble produce a sum over all 3-manifolds and how surgery is implemented by the matrix integral. The partition functions of the resulting 3d gravity theory agree with Virasoro TQFT (VTQFT) on a fixed, hyperbolic manifold. However, on non-hyperbolic geometries, our 3d gravity theory differs from VTQFT, leading to a difference in the eigenvalue statistics of the associated ensemble. As explained in [1], the Schwinger-Dyson (SD) equations of the matrix-tensor integral play a crucial role in understanding how gravity emerges in the limit that the ensemble localizes to exact CFT’s. We show how the SD equations can be translated into a combinatorial problem about 3-manifolds.

Journal of High Energy PhysicsVol. 2025(2)
Harvard University Press (US), University of Oxford (GB)
U.S. Department of Energy, CERN, Center of Mathematical Sciences and Applications, Harvard University, Science and Technology Facilities Council
Openalex Percentile: Top 1%
Black Holes and Theoretical Physics
18.70
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