We obtain two stationary solutions for an intense optical pulse propagating in a Kerr-effect nonlinear ring cavity using elliptic functions associated with a parameter $m$. The solutions may be associated with distinct phases of the system, the transition from one to the other being dictated by an energy ratio. Semiclassical quantization reveals excitations that are quantized rotational states for the spatially constant solution and $N$-particle bound states for the soliton solution. On invoking periodic boundary conditions, a constraint relating the number of particles, wavelength, and $m$ emerges. This constraint fundamentally modifies the binding energy of the soliton for a large range of $m$. At the phase transition point, the energy undergoes a discontinuity in both value and derivative, a conclusion that differs markedly from results of a mean-field calculation.
Read full abstract