Abstract

We study the Eigenstate Thermalization Hypothesis (ETH) in chaotic conformal field theories (CFTs) of arbitrary dimensions. Assuming local ETH, we compute the reduced density matrix of a ball-shaped subsystem of finite size in the infinite volume limit when the full system is an energy eigenstate. This reduced density matrix is close in trace distance to a density matrix, to which we refer as the ETH density matrix, that is independent of all the details of an eigenstate except its energy and charges under global symmetries. In two dimensions, the ETH density matrix is universal for all theories with the same value of central charge. We argue that the ETH density matrix is close in trace distance to the reduced density matrix of the (micro)canonical ensemble. We support the argument in higher dimensions by comparing the Von Neumann entropy of the ETH density matrix with the entropy of a black hole in holographic systems in the low temperature limit. Finally, we generalize our analysis to the coherent states with energy density that varies slowly in space, and show that locally such states are well described by the ETH density matrix.

Highlights

  • Introduction and outlineQuantum information plays an increasingly important role in our understanding and characterization of quantum matter

  • We continue the study of the Eigenstate Thermalization Hypothesis (ETH) in the context of Conformal Field Theories initiated in [1]

  • We proved that if ETH is satisfied at the level of individual local operators, the subsystem ETH follows

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Summary

Introduction and outline

Quantum information plays an increasingly important role in our understanding and characterization of quantum matter. We argue that the universal density matrix in the thermodynamic limit is close to the reduced Generalized Gibbs Ensemble (GGE) provided we can map all their conserved charges. In the limit that the central charge c goes to ∞, we show that all the μi = 0 and the universal density matrix becomes close in trace distance to the standard Gibbs state. This is consistent with previous results of [7, 11].2.

ETH density matrix and thermal states
Different ensembles
Equivalence of reduced density matrices
Two dimensional CFTs
Universal reduced density matrix
Renyi entropies
Generalized Gibbs ensembles
Matching with thermal density matrix in the infinite c limit
Higher dimensional CFTs
ETH density matrix
Entanglement entropy from ETH density matrix
Holographic theories
Local equilibrium
Time-dependent coherent states
Conclusions
A Rindler space: a convenient conformal frame
B Global descendants in two dimensions
C Thermodynamically relevant quasi-primaries
D One-point functions on a torus
E Perturbative Renyi entropies
F Twist operators
G Failure of perturbation theory for GGE
A Qi β μiμj 2
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