We consider perturbations of the one-dimensional cubic Schrödinger equation, under the form i ∂tψ+∂ 2x ψ+|ψ| 2 ψ−g(|ψ| 2 )ψ = 0. Under hypotheses on the function g that can be easily verified in some cases, we show that the linearized problem around a solitary wave does not have internal mode (nor resonance) and we prove the asymptotic stability of these solitary waves, for small frequencies.Theorem 2. Assume that hypotheses (H 1 ) and (H 2 ) are satisfied. For ω 0 small enough, there exists δ > 0 so that, for anyδ, if we let ψ be the solution of (1) with initial data ψ(0) = ψ 0 , then there exists β + ∈ R and ω + > 0 such that, for any bounded interval I ⊂ R,Remarks. A few remarks can be given about this result. Most of them are already in the paper [16] and shall not be recalled here.• The result is written with an "inf γ,σ " formulation. It can be stated in another way, which is the actual way the proof will be led: there exists• The proof will show that ω(t), ω + ∈ 0 , 3ω0 2 . In fact, we could show that, for any η > 0, δ can be chosen small enough such that ω(t), ω + ∈ (0 , ω 0 + η).