2022
DOI: 10.1007/jhep05(2022)060
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Holographic local operator quenches in BCFTs

Abstract: We present a gravity dual of local operator quench in a two-dimensional CFT with conformal boundaries. This is given by a massive excitation in a three-dimensional AdS space with the end of the world brane (EOW brane). Due to the gravitational backreaction, the EOW brane gets deformed in a nontrivial way. We show that the energy-momentum tensor and entanglement entropy computed from the gravity dual and from the BCFT in the large c limit match perfectly. Interestingly, this comparison avoids the folding of the… Show more

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Cited by 21 publications
(15 citation statements)
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“…If a conical defect is introduced in an AdS spacetime with an end-of-the-world brane, the brane will be bent due to the gravitational interaction. When the deficit angle exceeds a certain threshold, the brane will intersect itself [30,31,70,83]. Configurations with brane self-intersections indeed are solutions to the Einstein equation.…”
Section: Gravity Dual Of the Bcft On A Half Planementioning
confidence: 99%
See 1 more Smart Citation
“…If a conical defect is introduced in an AdS spacetime with an end-of-the-world brane, the brane will be bent due to the gravitational interaction. When the deficit angle exceeds a certain threshold, the brane will intersect itself [30,31,70,83]. Configurations with brane self-intersections indeed are solutions to the Einstein equation.…”
Section: Gravity Dual Of the Bcft On A Half Planementioning
confidence: 99%
“…except for the identity I. This assumption is often considered in the AdS/BCFT construction to model setups where there is no direct coupling between the brane and the matter fields [3,83]. Another context where such an assumption is often considered in discussions about the BCFT dual of the island model [19,22].…”
Section: Bootstrapping a Two-point Function On A Stripmentioning
confidence: 99%
“…Unlike the case in [21], our investigation can be regarded as a pseudo-entropy extension of the real-time evolution of the entanglement entropy after such local operator excitations [33]. In recent years, the time evolution of entanglement entropy for locally excited states has been widely studied, including rational CFTs [34][35][36], irrational CFTs [37], large-c CFTs [38,39], boundary CFTs [40], warped CFTs [41], CFTs at finite temperature [42], multiple local excitations [43], and holographic duals of the local excitations [44][45][46][47]. In 2d rational CFTs (RCFTs), it was found that the variation of nth Rényi entropy for locally primary excited states saturates to a constant equal to the logarithm of the quantum dimension of the local operator's conformal family [34][35][36].…”
Section: Jhep09(2022)094mentioning
confidence: 99%
“…Their holographic dual involves a dynamical geometry that can be obtained from the back-reaction of a massive particle (or generally a bulk field), which is dual to that local operator [19]. In particular, entanglement evolution in these states has been studied extensively in the context of quantum quenches [20][21][22][23][24][25][26][27], scrambling [28,29], quantum chaos [30][31][32][33] as well as bulk reconstruction in AdS/CFT [34][35][36]. Certainly, this family provides very important and analytically tractable data points in the "spacetime from entanglement" program.…”
Section: Introductionmentioning
confidence: 99%