Using the master equation approach, we investigate the stationary regime of a single-emitter laser: an incoherently pumped single two-level system interacting with a single cavity mode of finite finesse. We analyze the closed equation for the phase-averaged Glauber-Sudarshan P function and obtain its approximate solution. This solution has some advantages over the previous results. In particular, it describes conversion from the classical-like probability distribution to the oscillating quasi-probability when transition from weak- to strong-coupling regime takes place.
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