Abstract

We consider quantum many-body systems evolving under a time-independent Hamiltonian HH from a nonequilibrium initial state at time t=0t=0 towards a close-to-equilibrium state at time t=τt=τ. Subsequently, this state is slightly perturbed and finally propagated for another time period ττ under the inverted Hamiltonian −H-H. The entire procedure may also be viewed as an imperfect time inversion or "echo dynamics". We unravel a remarkable persistence of such dynamics with respect to the observable deviations of the time-dependent expectation values from the equilibrium expectation value: For most perturbations, the deviations in the final state are essentially independent of the inversion time point ττ. Our quantitative analytical predictions compare very well with exact numerical results.

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