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      Holographic entanglement entropy and the extended phase structure of STU black holes

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          Abstract

          We study the extended thermodynamics, obtained by considering the cosmological constant as a thermodynamic variable, of STU black holes in 4-dimensions in the fixed charge ensemble. The associated phase structure is conjectured to be dual to an RG-flow on the space of field theories. We find that for some charge configurations the phase structure resembles that of a Van der Waals gas: the system exhibits a family of first order phase transitions ending in a second order phase transition at a critical temperature. We calculate the holographic entanglement entropy for several charge configurations and show that for the cases where the gravity background exhibits Van der Waals behavior, the entanglement entropy presents a transition at the same critical temperature. To further characterize the phase transition we calculate appropriate critical exponents and show that they coincide. Thus, the entanglement entropy successfully captures the information of the extended phase structure. Finally, we discuss the physical interpretation of the extended space in terms of the boundary QFT and construct various holographic heat engines dual to STU black holes.

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          Charged AdS Black Holes and Catastrophic Holography

          We compute the properties of a class of charged black holes in anti-de Sitter space-time, in diverse dimensions. These black holes are solutions of consistent Einstein-Maxwell truncations of gauged supergravities, which are shown to arise from the inclusion of rotation in the transverse space. We uncover rich thermodynamic phase structures for these systems, which display classic critical phenomena, including structures isomorphic to the van der Waals-Maxwell liquid-gas system. In that case, the phases are controlled by the universal `cusp' and `swallowtail' shapes familiar from catastrophe theory. All of the thermodynamics is consistent with field theory interpretations via holography, where the dual field theories can sometimes be found on the world volumes of coincident rotating branes.
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            Black Hole Enthalpy and an Entropy Inequality for the Thermodynamic Volume

            In a theory where the cosmological constant \(\Lambda\) or the gauge coupling constant \(g\) arises as the vacuum expectation value, its variation should be included in the first law of thermodynamics for black holes. This becomes \(dE= TdS + \Omega_i dJ_i + \Phi_\alpha d Q_\alpha + \Theta d \Lambda\), where \(E\) is now the enthalpy of the spacetime, and \(\Theta\), the thermodynamic conjugate of \(\Lambda\), is proportional to an effective volume \(V = -\frac{16 \pi \Theta}{D-2}\) "inside the event horizon." Here we calculate \(\Theta\) and \(V\) for a wide variety of \(D\)-dimensional charged rotating asymptotically AdS black hole spacetimes, using the first law or the Smarr relation. We compare our expressions with those obtained by implementing a suggestion of Kastor, Ray and Traschen, involving Komar integrals and Killing potentials, which we construct from conformal Killing-Yano tensors. We conjecture that the volume \(V\) and the horizon area \(A\) satisfy the inequality \(R\equiv ((D-1)V/{\cal A}_{D-2})^{1/(D-1)}\, ({\cal A}_{D-2}/A)^{1/(D-2)}\ge1\), where \({\cal A}_{D-2}\) is the volume of the unit \((D-2)\)-sphere, and we show that this is obeyed for a wide variety of black holes, and saturated for Schwarzschild-AdS. Intriguingly, this inequality is the "inverse" of the isoperimetric inequality for a volume \(V\) in Euclidean \((D-1)\) space bounded by a surface of area \(A\), for which \(R\le 1\). Our conjectured {\it Reverse Isoperimetric Inequality} can be interpreted as the statement that the entropy inside a horizon of a given "volume" \(V\) is maximised for Schwarzschild-AdS. The thermodynamic definition of \(V\) requires a cosmological constant (or gauge coupling constant). However, except in 7 dimensions, a smooth limit exists where \(\Lambda\) or \(g\) goes to zero, providing a definition of \(V\) even for asymptotically-flat black holes.
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              Cosmological constant as confining U(1) charge in two-dimensional dilaton gravity

              The cosmological constant is treated as a thermodynamical parameter in the framework of two-dimensional dilaton gravity. We find that the cosmological constant behaves as a U(1) charge with a confining potential, and that such potentials require a novel Born-Infeld boundary term in the action. The free energy and other thermodynamical quantities of interest are derived, from first principles, in a way that is essentially model-independent. We discover that there is always a Schottky anomaly in the specific heat and explain its physical origin. Finally, we apply these results to specific examples, like Anti-de Sitter-Schwarzschild-Tangherlini black holes, Banados-Teitelboim-Zanelli black holes and the Jackiw-Teitelboim model.
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                Author and article information

                Journal
                2015-07-22
                2015-10-08
                Article
                1507.06069
                da179941-6455-4d99-9802-206f3f7a164c

                http://arxiv.org/licenses/nonexclusive-distrib/1.0/

                History
                Custom metadata
                UTTG-14-15, TCC-005-15
                JHEP 1509 (2015) 184
                35 pages, multiple figures. v3: matches published version
                hep-th gr-qc

                General relativity & Quantum cosmology,High energy & Particle physics
                General relativity & Quantum cosmology, High energy & Particle physics

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