Abstract:
We deal with the nonlinear lattice i˙ψn+(1−|ψn|2)(ψn+1+ψn−1−2ψn)+2(ρ2−|ψn|2)ψn+γnψn=0
subject to the finite density boundary conditions. It is shown that it is integrable by means of the inverse scattering technique. Soliton solutions undergo periodic motion with the frequency γ. Small amplitude limit of the model is discussed.