We have studied the behavior of two symmetrically coupled Lorenz systems in the parameter space where the uncoupled systems correspond to the bad-cavity limit of the single-mode laser model. The differential equations show that the threshold for the appearance of a strange attractor in the coupled system drops below the uncoupled value, exhibits a minimum at {β}=0.5, and then increases rapidly as {β}{→}0.7. We have also studied the use of coupled logistic cusp maps for predicting the initial drop in the second laser threshold. The results show good qualitative agreement for low {β} values ({β}<0.25).
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Lawandy et al. (1986) studied this question.
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