A non-linear medium interacting with two intense counterpropagating beams can give rise to a four-wave mixing gain for a probe wave [1]. This gain can be sufficient to observe oscillation when the medium is placed inside a cavity [2], or placed in front of a single mirror [3] or even in free space without any mirrors [4].
We have developed a theory for nondegenerate oscillations in optical resonators containing an intracavity phase-conjugate element. The phase-conjugate element consists of a nonlinear transparent medium that is pumped externally by a pair of counterpropagating laser beams of the same frequency and intensity. Phase conjugation of an input beam of slightly different frequency occurs because of nondegenerate four-wave mixing. The theory takes into account linear absorption (or gain) in the medium and is applied to study the threshold behavior of phase-conjugate oscillators. For the special case of no conventional mirrors, the phase-conjugate oscillator reduces to an ordinary phase-conjugate mirror, and our general formulation yields the results of previous studies. Our analysis shows that the parametric gain required for oscillation increases (or decreases) as a result of linear absorption (or gain) in the medium, and oscillation can occur at a frequency different from that of the pump beams in the presence of large linear gain (or loss). The effects of linear absorption (or gain) on the filter operation are also examined.
The physics of Raman-type self-oscillations in highly dispersive saturable two-level-medium devices is revisited by using the gain and reflectivity matrices. The probe gain when two identical pumps counterpropagate through a two-level system is demonstrated to be very different from the gain for a probe in a one-way device, and typically peaked near a frequency twice the one-way Rabi frequency, while multiwave mixing displays a generalized mirror behavior of the atomic cell. The multimode instability in a Fabry-P\'erot interferometer is also discussed and shown to be mainly a result of counterpropagating probe coupling while the coupling between copropagating probe and idler is negligible.
Oscillation in a cavity using a four-wave mixing amplifier has been recently observed. This type of oscillator has properties very similar to those of a parametric oscillator but for the fact that the gain mechanism is due to a X(3) non linear susceptibility rather than a X(2). One of the consequences of this difference is that the gain mechanism and the intensity dependent refractive index (which also depends on X(3)) appears at the same order of perturbation and should be simultaneously considered in the analysis of the oscillation. In particular, this leads to the prediction that such an oscillator is intrinsically bistable.