Abstract
An Ar + laser driven across the threshold region by a slow variation of the cavity losses displays a delayed bifurcation and easily observable lags relative to the true steady state of the system. The delayed bifurcation is the result of a dynamical stabilization of the zero-field state that persists even when the cavity losses are swept at a rate which is smaller, by several orders of magnitudes, than all the other decay rates of the system. These results are in good qualitative agreement with the predictions of a simple theoretical model.
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