After a quench to a sine-square deformed Hamiltonian, symmetry-resolved entanglement entropy grows as log t, with a subleading charge-dependent correction that breaks equipartition.
Holographic Quenches in a Confined Phase
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abstract
We investigate quenches of holographic theories in a confined phase, where the energy injected is insufficient to reach the deconfined phase. In such quenches, thermalization is not associated with gravitational collapse and the formation of a black hole. Nevertheless, we attempt to characterize the late-time state of this scenario. We check a number of notions of thermalization that do not require horizon formation, and find no evidence for thermalization in our chosen parameters and initial states, even in the weakest sense. We find that the post-quench behaviour of both local and nonlocal observables exhibit oscillatory behaviour rather than decaying towards equilibrium. We generally find that the response of the nonlocal observables is smoother than that of the local ones. We discuss mechanisms which generate such smoothing, as well as "beats" which appear in the time-dependence of the nonlocal operators for certain classes of quenches. When tuning the quench parameters such that the smoothing is ineffective, we are able to perform "entanglement spectroscopy", recovering the spectrum of the confined phase of the theory from the time dependence of the entanglement entropy, as well as other nonlocal observables.
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Symmetry resolved entanglement entropy after an inhomogeneous quench
After a quench to a sine-square deformed Hamiltonian, symmetry-resolved entanglement entropy grows as log t, with a subleading charge-dependent correction that breaks equipartition.