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      Black branes in asymptotically Lifshitz spacetime and viscosity/entropy ratios in Horndeski gravity

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          Abstract

          We investigate black brane solutions in asymptotically Lifshitz spacetime in 3+1-dimensional Horndeski gravity, which parameters are related to the cosmological constant as \(\alpha=\gamma\Lambda\) and depend on arbitrary values of the dynamical critical exponent \(z\) since \(\Lambda=-(1+2z)/L^{2}\). For the case \(z=1\) we recover black brane solutions in asymptotically AdS\(_{4}\) spacetime. We also investigate the shear viscosity in the 2+1-dimensional dual boundary field theory via holographic correspondence. We show that for arbitrary values of AdS radius \(L\), only two specific critical exponents are allowed: \(z= -0.3\) or \(z= 3.3\). At the former value, we find that the bound for viscosity to entropy density ratio \(\eta/s\geq1/(4\pi)\) is violated.

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          Viscosity in Strongly Interacting Quantum Field Theories from Black Hole Physics

          The ratio of shear viscosity to volume density of entropy can be used to characterize how close a given fluid is to being perfect. Using string theory methods, we show that this ratio is equal to a universal value of \(\hbar/4\pi k_B\) for a large class of strongly interacting quantum field theories whose dual description involves black holes in anti--de Sitter space. We provide evidence that this value may serve as a lower bound for a wide class of systems, thus suggesting that black hole horizons are dual to the most ideal fluids.
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            Gauge Theory Correlators from Non-Critical String Theory

            We suggest a means of obtaining certain Green's functions in 3+1-dimensional \({\cal N} = 4\) supersymmetric Yang-Mills theory with a large number of colors via non-critical string theory. The non-critical string theory is related to critical string theory in anti-deSitter background. We introduce a boundary of the anti-deSitter space analogous to a cut-off on the Liouville coordinate of the two-dimensional string theory. Correlation functions of operators in the gauge theory are related to the dependence of the supergravity action on the boundary conditions. From the quadratic terms in supergravity we read off the anomalous dimensions. For operators that couple to massless string states it has been established through absorption calculations that the anomalous dimensions vanish, and we rederive this result. The operators that couple to massive string states at level \(n\) acquire anomalous dimensions that grow as \(2\left (n g_{YM} \sqrt {2 N} )^{1/2}\) for large `t Hooft coupling. This is a new prediction about the strong coupling behavior of large \(N\) SYM theory.
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              Large N Field Theories, String Theory and Gravity

              We review the holographic correspondence between field theories and string/M theory, focusing on the relation between compactifications of string/M theory on Anti-de Sitter spaces and conformal field theories. We review the background for this correspondence and discuss its motivations and the evidence for its correctness. We describe the main results that have been derived from the correspondence in the regime that the field theory is approximated by classical or semiclassical gravity. We focus on the case of the N=4 supersymmetric gauge theory in four dimensions, but we discuss also field theories in other dimensions, conformal and non-conformal, with or without supersymmetry, and in particular the relation to QCD. We also discuss some implications for black hole physics.
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                Author and article information

                Journal
                20 January 2019
                Article
                1901.06770
                5b942ce9-354a-4608-83ee-19ee8532407a

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

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                Custom metadata
                Latex, 19 pages, 1 figure and 1 table
                hep-th gr-qc

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

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