Entanglement Renyi entropies in holographic theories
By M. Headrick. 2010
661 citations recorded by the source corpus.
Ryu and Takayanagi conjectured a formula for the entanglement (von Neumann) entropy of an arbitrary spatial region in an arbitrary holographic eld theory. The von Neumann entropy is a special case of a more general class of entropies called R enyi entropies. Using Euclidean gravity, Fursaev computed the entanglement R enyi entropies (EREs) of an arbitrary spatial region in an arbitrary holographic eld theory, and thereby derived the RT formula. We point out, however, that his EREs are incorrect, since his putative saddle points do not in fact solve the Einstein equation. We remedy this situation in the case of two-dimensional CFTs, considering regions consisting of one or two intervals. For a single interval, the EREs are known for a general CFT; we reproduce them using gravity. For two intervals, the RT formula predicts a phase transition in the entanglement entropy as a function of their separation, and that the mutual information between the intervals vanishes for separations larger than the phase transition point. By computing EREs using gravity and CFT techniques, we nd evidence supporting both predictions. We also nd evidence that large-N symmetric-product theories have the same EREs as holographic ones.
Subfields: Astronomy and Astrophysics, Nuclear and High Energy Physics
View Paper: https://www.semanticscholar.org/paper/bedd6e2046a56b922947d1045624fa2752d9a085
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Citations in the corpus
- A Holographic View on Physics out of Equilibrium (2010, positive): “This is indeed supported by the proposal 56 Justification of this remarkable statement was subsequently provided in [210] using replica trick to evaluate entanglement Renyi entropies; although an error in this derivation was recently pointed out by [211], the correction nevertheless gives further ev”
- Quantum extremal islands made easy. Part II. Black holes on the brane (2020, background): “As emphasized in [1], the transition between the phase without an island and that with the island is nothing more than the usual transition between different classes of RT surfaces [73–75] – see figure 2.”
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- Holographic c-theorems in arbitrary dimensions (2010, result): “As emphasized in [75], the derivation presented in [76] is flawed and, for example, leads to incorrect results in holographic calculations of Renyi entropies.”
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- Quantum extremal islands made easy. Part I. Entanglement on the brane (2020, neutral): “, [110].”
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