4.4 Article

Symmetry-resolved entanglement for excited states and two entangling intervals in AdS3/CFT2

期刊

JOURNAL OF HIGH ENERGY PHYSICS
卷 -, 期 12, 页码 -

出版社

SPRINGER
DOI: 10.1007/JHEP12(2021)104

关键词

AdS-CFT Correspondence; Gauge-gravity correspondence

资金

  1. Deutsche Forschungsgemeinschaft (DFG, German Research Foundation) [EXC 2147, 390858490]
  2. China Scholarship Council
  3. [258499086 - SFB 1170]

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The authors tested the proposal of [1] for holographic computation of charged moments and symmetry-resolved entanglement entropy in different excited states, as well as for two entangling intervals. The results showed equipartition of entanglement between different charge sectors in all cases.
We test the proposal of [1] for the holographic computation of the charged moments and the resulting symmetry-resolved entanglement entropy in different excited states, as well as for two entangling intervals. Our holographic computations are performed in U(1) Chern-Simons-Einstein-Hilbert gravity, and are confirmed by independent results in a conformal field theory at large central charge. In particular, we consider two classes of excited states, corresponding to charged and uncharged conical defects in AdS(3). In the conformal field theory, these states are generated by the insertion of charged and uncharged heavy operators. We employ the monodromy method to calculate the ensuing four-point function between the heavy operators and the twist fields. For the two-interval case, we derive our results on the AdS and the conformal field theory side, respectively, from the generating function method of [1], as well as the vertex operator algebra. In all cases considered, we find equipartition of entanglement between the different charge sectors. We also clarify an aspect of conformal field theories with a large central charge and (u) over cap (1)(k) Kac-Moody symmetry used in our calculations, namely the factorization of the Hilbert space into a gravitational Virasoro sector with large central charge, and a (u) over cap (1) (k) Kac-Moody sector.

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