Abstract
We consider a -symmetric ladder-shaped optical array consisting of a chain of waveguides with gain coupled to a parallel chain of waveguides with loss. All waveguides have the focusing Kerr nonlinearity. The array supports two co-existing solitons, an in-phase and an antiphase one, and each of these can be centred either on a lattice site or midway between two neighbouring sites. We show that both bond-centred (i.e. intersite) solitons are unstable regardless of their amplitudes and parameters of the chain. The site-centred in-phase soliton is stable when its amplitude lies below a threshold that depends on the coupling and gain–loss coefficient. The threshold is lowest when the gain-to-gain and loss-to-loss coupling constant in each chain is close to the interchain gain-to-loss coupling coefficient. The antiphase site-centred soliton in the strongly-coupled chain or in a chain close to the -symmetry breaking point, is stable when its amplitude lies above a critical value and unstable otherwise. The instability growth rate of solitons with small amplitude is exponentially small in this parameter regime; hence the small-amplitude solitons, though unstable, have exponentially long lifetimes. On the other hand, the antiphase soliton in the weakly or moderately coupled chain and away from the -symmetry breaking point, is unstable when its amplitude falls in one or two finite bands. All amplitudes outside those bands are stable.
Highlights
In soliton-bearing optical systems, weak dissipative losses are typically compensated by the application of a resonant pump
Dissipative solitons in systems with competing linear and nonlinear gain and loss — systems modelled by the Ginsburg-Landau equations — are inflexible
It is important to emphasise that the region described by the inequalities (6.8) and (6.6) constitutes only a part of the full stability domain of the antiphase soliton; see Fig 13(a)
Summary
In soliton-bearing optical systems, weak dissipative losses are typically compensated by the application of a resonant pump. The balance of nonlinearity and diffraction or dispersion singles out a one-parameter family of solitons, while the competition of gain and loss fixes a particular member of the family [2]. With a judicious choice of coupling, the combined system with gain and loss will contain, as its scalar reduction, the unperturbed nonlinear Schrodinger equation As a result, this PT -symmetric system will support families of solitons with continuously variable amplitudes, phases, and velocities. We will show that stability properties of the in-phase and antiphase site-centred soliton are completely determined just by two combinations of C, γ and the soliton’s amplitude.
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