Periodic driving induces DQPTs in the 1D Ising model via resonance within a phase (linked to Floquet topology) or low-frequency crossing of the critical point due to energy degeneracy.
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Thermalization after a quench in the Hubbard-Holstein model occurs via sharp fronts in real time and DMFT iteration space, with electron fronts appearing earlier than phonon fronts at weak coupling.
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Dynamical Phase Transitions in Periodically Driving 1D Ising Model
Periodic driving induces DQPTs in the 1D Ising model via resonance within a phase (linked to Floquet topology) or low-frequency crossing of the critical point due to energy degeneracy.
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Thermalization Fronts in the Hubbard-Holstein Model
Thermalization after a quench in the Hubbard-Holstein model occurs via sharp fronts in real time and DMFT iteration space, with electron fronts appearing earlier than phonon fronts at weak coupling.