Exact steady states are derived for interacting dissipative fermionic systems with hidden time-reversal symmetry, revealing a first-order particle density phase transition that survives finite dissipation.
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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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Exact steady states of interacting driven dissipative fermionic systems with hidden time-reversal symmetry
Exact steady states are derived for interacting dissipative fermionic systems with hidden time-reversal symmetry, revealing a first-order particle density phase transition that survives finite dissipation.
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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.