Abstract

We explore the structures of light cone and Regge limit singularities of n-point Virasoro conformal blocks in c > 1 two-dimensional conformal field theories with no chiral primaries, using fusion matrix approach. These CFTs include not only holographic CFTs dual to classical gravity, but also their full quantum corrections, since this approach allows us to explore full 1/c corrections. As the important applications, we study time dependence of Renyi entropy after a local quench and out-of-time ordered correlator (OTOC) at late time.We first show that, the n-th (n > 2) Renyi entropy after a local quench in our CFT grows logarithmically at late time, for any c and any conformal dimensions of excited primary. In particular, we find that this behavior is independent of c, contrary to the expectation that the finite c correction fixes the late time Renyi entropy to be constant. We also show that the constant part of the late time Renyi entropy is given by a monodromy matrix.We also investigate OTOCs by using the monodromy matrix. We first rewrite the monodromy matrix in terms of fusion matrix explicitly. By this expression, we find that the OTOC decays exponentially in time, and the decay rates are divided into three patterns, depending on the dimensions of external operators. We note that our result is valid for any c > 1 and any external operator dimensions. Our monodromy matrix approach can be generalized to the Liouville theory and we show that the Liouville OTOC approaches constant in the late time regime.We emphasize that, there is a number of other applications of the fusion and the monodromy matrix approaches, such as solving the conformal bootstrap equation. Therefore, it is tempting to believe that the fusion and monodromy matrix approaches provide a key to understanding the AdS/CFT correspondence.

Highlights

  • Introduction & summaryThe AdS/CFT correspondence is a useful tool to investigate quantum gravity in terms of CFT

  • We show that the constant part of the late time Renyi entropy is given by a monodromy matrix

  • Our monodromy matrix approach can be generalized to the Liouville theory and we show that the Liouville of-time ordered correlator (OTOC) approaches constant in the late time regime

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Summary

Introduction & summary

The AdS/CFT correspondence is a useful tool to investigate quantum gravity in terms of CFT. The most simplest CFTs in this class are unitary, compact CFTs with central charge c > 1 and without chiral primaries (no extra currents apart from the Virasoro current), which we call pure CFTs.. The most simplest CFTs in this class are unitary, compact CFTs with central charge c > 1 and without chiral primaries (no extra currents apart from the Virasoro current), which we call pure CFTs.1,2 These CFTs are often considered in the context of holography (for e.g., [1, 2]); we do not know the explicit construction of such CFTs yet, that is, we have no example of a pure CFT. We determine the generic behavior of the Renyi entanglement entropy of locally excited state and late time out-of-time ordered correlator

Virasoro block from fusion and monodromy approaches
Geometric part of entanglement growth
Topological part of entanglement growth
Out-of-time ordered correlator
Light cone bootstrap
Light-cone conformal bootstrap
Twist spectrum as two particle state in AdS3
Singularity of n-point block
Regge singularity from monodromy matrix
Phase factor
General solutions to Zamolodchikov recursion relation
Bulk interpretation of light cone and Regge limit singularities
Renyi entropy after local quench
Renyi entropy from twist frame
Entanglement entropy and Renyi entropy in large c limit
Q αh hH and γσn
Renyi entropy in pure CFT
Renyi entropy in RCFT
Renyi entropy in Liouville CFT
Late time regime
Non-vacuum contribution in late time
Q2 log
OTOC in Liouville CFT
Discussion
A Explicit form of fusion matrix
B Singularity of n-point block
C Monodromy matrix in Ising model
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