Abstract
The unabbreviated Lamb semiclassical equations for the case of three interacting modes are numerically solved for a variety of laser parameters. Steady-state solutions are obtained for the amplitudes, beat frequencies, and time development of the modes by using the Kutta-Merson method of integration. It is found that for some solutions the relative phase angle ψ becomes constant, and so it is clear under what conditions self-locking is possible. When the modes are unlocked, the value of ψ varies with time even after the steady-state amplitudes have been achieved. Comparison is made with the locking criteria predicted by approaches to the theory where approximations have been made. A physical interpretation is given for the presence or absence of self-locking in terms of competition and of the ratio ΔΔνD. Some general rules are established for the behavior of the rise time and delay of the onset of oscillation of the three modes.

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