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      Modular Hamiltonians for Deformed Half-Spaces and the Averaged Null Energy Condition

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          Abstract

          We study modular Hamiltonians corresponding to the vacuum state for deformed half-spaces in relativistic quantum field theories on \(\mathbb{R}^{1,d-1}\). We show that in addition to the usual boost generator, there is a contribution to the modular Hamiltonian at first order in the shape deformation, proportional to the integral of the null components of the stress tensor along the Rindler horizon. We use this fact along with monotonicity of relative entropy to prove the averaged null energy condition in Minkowski space-time. This subsequently gives a new proof of the Hofman-Maldacena bounds on the parameters appearing in CFT three-point functions. Our main technical advance involves adapting newly developed perturbative methods for calculating entanglement entropy to the problem at hand. These methods were recently used to prove certain results on the shape dependence of entanglement in CFTs and here we generalize these results to excited states and real time dynamics. We also discuss the AdS/CFT counterpart of this result, making connection with the recently proposed gravitational dual for modular Hamiltonians in holographic theories.

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          Energy conditions and spacetime singularities

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            Geodesic focusing, energy conditions and singularities

            A. Borde (1987)
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              A finite entanglement entropy and the c-theorem

              The trace over the degrees of freedom located in a subset of the space transforms the vacuum state into a mixed density matrix with non zero entropy. This is usually called entanglement entropy, and it is known to be divergent in quantum field theory (QFT). However, it is possible to define a finite quantity F(A,B) for two given different subsets A and B which measures the degree of entanglement between their respective degrees of freedom. We show that the function F(A,B) is severely constrained by the Poincare symmetry and the mathematical properties of the entropy. In particular, for one component sets in two dimensional conformal field theories its general form is completely determined. Moreover, it allows to prove an alternative entropic version of the c-theorem for 1+1 dimensional QFT. We propose this well defined quantity as the meaningfull entanglement entropy and comment on possible applications in QFT and the black hole evaporation problem.
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                Author and article information

                Journal
                2016-05-25
                Article
                1605.08072
                e6f14887-2f03-4594-80df-b52b4f516a51

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

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                Custom metadata
                40 pages, 5 figures
                hep-th gr-qc quant-ph

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

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