Quenching a mixed-field Ising chain from paramagnetic to ferromagnetic parameters makes small subsystems display strong non-Markovian, memory-retaining dynamics, while the reverse quench is nearly Markovian.
Open-systems tools for non-thermalizing closed quantum systems
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abstract
We design several examples of constrained, symmetric quantum circuit dynamics that generate non-equilibrium steady states. The qubit networks maintain local memory of the initial conditions and display inhomogeneous subsystem dynamics over long times, clearly distinguishable from approximately thermalizing networks of the same size. Each network can be described as an ensemble of open systems, a collection of qubits evolving with phase-covariant dynamics. Constraints from the conservation law and global unitary dynamics of the entire network bound the distribution of single-qubit dynamics in the ensemble, but different steady states are distinguishable by several measures. We quantify the distance of the steady states from the homogeneous steady state and further characterize them using the complexity of their mutual information networks, the volume of state space explored, a thermodynamic utility measure using extractable work, and correlated structure in the occurrence of non-completely positive qubit propagator maps.
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Non-Markovianity of subsystem dynamics in isolated quantum many-body systems
Quenching a mixed-field Ising chain from paramagnetic to ferromagnetic parameters makes small subsystems display strong non-Markovian, memory-retaining dynamics, while the reverse quench is nearly Markovian.