In a solvable random-circuit model, all higher-order OTOCs decay at the same rate λ^{2t} (λ from a single-particle channel), and their late-time values match the free-cumulant decomposition predicted by full ETH.
Steady-state dynamical mean field theory based on influence functional matrix product states
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abstract
We implement the recently developed influence functional matrix product states approach as impurity solver in equilibrium and nonequilibrium dynamical mean field theory (DMFT) calculations of the single-band Hubbard model. The method yields numerically exact descriptions of metallic states without sharp spectral features, at a moderate numerical cost. Systems with narrow quasiparticle or spin-polaron peaks, as well as low-temperature Mott insulators provide more challenges, since these simulations require long time contours or high bond dimensions. A promising field of application is the DMFT simulation of nonequilibrium steady states, which we demonstrate with results for photo-doped Mott systems with long-lived doublon and holon populations.
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Free Probability in a Minimal Quantum Circuit Model
In a solvable random-circuit model, all higher-order OTOCs decay at the same rate λ^{2t} (λ from a single-particle channel), and their late-time values match the free-cumulant decomposition predicted by full ETH.