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Holographic RG flows in a 3d gauged supergravity at finite temperature

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arxiv 2405.06515 v2 pith:SU3RM6E3 submitted 2024-05-10 hep-th gr-qc

classification hep-thgr-qc
keywords pointssolutionsblackfixedflowsholographicsystemtemperature
verification ladder T0 review T1 audit T2 compute T3 formal
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abstract

In this paper we consider finite-temperature holographic RG flows in $D=3$ $\mathcal{N}=(2,0)$ gauged truncated supergravity coupled to a sigma model with a hyperbolic target space. In the context of the holographic duality, fixed points (CFTs) at finite temperature are described by AdS black holes. We come from the gravity EOM to a 3d autonomous dynamical system, which critical points can be related to fixed points of dual field theories. Near-horizon black hole solutions correspond to infinite points of this system. We use Poincar\'e transformations to project the system on $\mathbf{R}^3$ into the 3d unit cylinder such that the infinite points are mapped onto the boundary of the cylinder. We explore numerically the space of solutions. We show that the exact RG flow at zero temperature is the separatrix for asymptotically AdS black hole solutions if the potential has one extremum, while for the potential with three extrema the separatrices are RG flows between AdS fixed points. We find near-horizon analytical solutions for asymptotically AdS black holes using the dynamical equations. We also present a method for constructing full analytical solutions.

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Cited by 2 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score. Full citation record

  1. Janus and RG-interfaces in minimal 3d gauged supergravity

    hep-th 2024-12 conditional novelty 6.0 of 10

    New numerical interface solutions in a minimal 3d supergravity model satisfy the proposed universal inequality between transmission and entanglement.

  2. More on thermal holographic RG flows in a 3D gauged supergravity

    hep-th 2024-12 conditional novelty 5.0 of 10

    In a 3D gauged supergravity, thermal holographic RG flows come in monotonic and non-monotonic classes, with a special analytic class where the metric is exactly BTZ and the scalar is hypergeometric.

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