Optical-parametric-oscillator solitons driven by the third harmonic

Abstract

We introduce a model of a lossy second-harmonic-generating (χ (2) ) cavity externally pumped at the third harmonic, which gives rise to driving terms of a new type, corresponding to a cross-parametric gain. The equation for the fundamental-frequency (FF) wave may also contain a quadratic self-driving term, which is generated by the cubic nonlinearity of the medium. Unlike previously studied phase-matched models of χ (2) cavities driven at the second harmonic (SH) or at FF, the present one admits an exact analytical solution for the soliton, at a special value of the gain parameter. Two families of solitons are found in a numerical form, and their stability area is identified through numerical computation of the perturbation eigenvalues (stability of the zero solution, which is a necessary condition for the soliton's stability, is investigated in an analytical form). One family is a continuation of the special analytical solution.At given values of parameters, one soliton is stable and the other one is not; they swap their stability at a critical value of the mismatch parameter. The stability of the solitons is also verified in direct simulations, which demonstrate that the unstable pulse rearranges itself into the stable one, or into a delocalized state, or decays to zero. A soliton which was given an initial boost C starts to move but quickly comes to a halt, if the boost is smaller than a critical value C cr . If C > C cr , the boost destroys the soliton (sometimes, through splitting into two secondary pulses). Interactions between initially separated solitons are investigated too. It is concluded that stable solitons always merge into a single one. In the system with weak loss, it appears in a vibrating form, slowly relaxing to the static shape. With stronger loss, the final soliton emerges in the stationary form.

Stability and dynamics of transverse field structures in the optical parametric oscillator near resonance signal detuning

“…Figure 11 demonstrates this evolution. And as with previous localized solutions, (17) can destabilize and form structures observed previously. For instance, figure 12 demonstrates a similar structure to that of figure 4.…”

“…Although this is not an exact solution for all X and Y, it holds along a periodic lattice. Numerically integrating (6) with the initial condition (17) can quickly settle to a steadystate solution which is perturbatively close to that constructed. Figure 11 demonstrates this evolution.…”

“…In all cases, of greatest scientific interest is the stable solutions and structures which arise in the OPO cavity. A myriad of stable solutions have been observed including localized pulse-like solutions [5,17,23], domain-walls (fronts) [4,13,23] and such patterns as rolls, hexagons and zig-zags [10]. Often, bifurcation studies can be conducted for these stable steady-state patterns as a function of the OPO cavity parameters [9].…”

Stability and interactions of transverse field structures in optical parametric oscillators near resonance detuning

“…For instance, in a singly resonant OPO cavity the Ginzburg-Landau description is appropriate [12,13] whereas in a doubly resonant OPO cavity the Swift-Hohenberg description is valid [12,13]. Observed OPE/OPO solutions include localized pulse-like solutions [5,19,20], domain-walls (fronts) [4,14,[20][21][22], labyrinths [22] oscillatory (Hopf) structures [23], and such patterns as rolls, hexagons and zig-zags [10].…”