Phases of scrambling in eigenstates
arXiv:1903.03143 · doi:10.21468/SciPostPhys.7.1.003
Abstract
We use the monodromy method to compute expectation values of an arbitrary number of light operators in finitely excited ("heavy") eigenstates of holographic 2D CFT. For eigenstates with scaling dimensions above the BTZ threshold, these behave thermally up to small corrections, with an effective temperature determined by the heavy state. Below the threshold we find oscillatory and not decaying behavior. As an application of these results we compute the expectation of the out-of-time order arrangement of four light operators in a heavy eigenstate, i.e. a six-point function. Above the threshold we find maximally scrambling behavior with Lyapunov exponent . Below threshold we find that the eigenstate OTOC shows persistent harmonic oscillations.
25 pages. 2 figures. v2 references added. v3 minor typos fixed
References in corpus (8)
- Black holes as mirrors: quantum information in random subsystems
- Holography from Conformal Field Theory
- Universal Spectrum of 2d Conformal Field Theory in the Large c Limit
- Holographic Entanglement Entropy from 2d CFT: Heavy States and Local Quenches
- Quantum Entanglement of Localized Excited States at Finite Temperature
- Eigenstate thermalization in the Sachdev-Ye-Kitaev model
- A Matrix Model for Black Hole Thermalization
- From Conformal Blocks to Path Integrals in the Vaidya Geometry