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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A quantum instanton method based on quasiprobability dynamics describes stationary states and asymptotic relaxation rates for large-spin collective systems, outperforming the Wigner approach by accounting for non-Gaussian fluctuations.
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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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Quantum instanton approach to metastable collective spins
A quantum instanton method based on quasiprobability dynamics describes stationary states and asymptotic relaxation rates for large-spin collective systems, outperforming the Wigner approach by accounting for non-Gaussian fluctuations.