In the subradiant regime of a bad-cavity laser, a dissipative phase transition maps to a switch from detailed-balance Markov chains to ones with time-asymmetric currents and N-scaling entropy production, producing observable self-pulsing.
Pfeifer,The Lie Algebras su(N), An Introduction (Birkh¨ auser, 2003)
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Dynamical aspects of steady-state subradiance: Detailed balance and its breakdown
In the subradiant regime of a bad-cavity laser, a dissipative phase transition maps to a switch from detailed-balance Markov chains to ones with time-asymmetric currents and N-scaling entropy production, producing observable self-pulsing.