Abstract
We consider a quantum quench in a finite system of length described by a -dimensional conformal field theory (CFT), of central charge , from a state with finite energy density corresponding to an inverse temperature . For times such that the reduced density matrix of a subsystem of length is exponentially close to a thermal density matrix. We compute exactly the overlap of the state at time with the initial state and show that in general it is exponentially suppressed at large . However, for minimal models with (more generally, rational CFTs), at times which are integer multiples of (for periodic boundary conditions, for open boundary conditions) there are (in general, partial) revivals at which is , leading to an eventual complete revival with . There is also interesting structure at all rational values of , related to properties of the CFT under modular transformations. At early times there is a universal decay . The effect of an irrelevant nonintegrable perturbation of the CFT is to progressively broaden each revival at by an amount .
- Received 17 March 2014
DOI:https://doi.org/10.1103/PhysRevLett.112.220401
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