Time quasi-periodic unbounded perturbations of Schrodinger operators and KAM methods

We eliminate by KAM methods the time dependence in a class of linear differential equations in l(2) subject to an unbounded, quasi-periodic forcing. This entails the pure-point nature of the Floquet spectrum of the operator H-0 + epsilonP(omegat) for epsilon small. Here H-0 is the one-dimensional Schrodinger operator p(2) + V, V(x) similar to \x\(alpha), alpha > 2 for \x\ --> infinity, the time quasi-periodic perturbation P may grow as \x\(beta), beta < (alpha - 2)/2, and the frequency vector omega is non resonant. The proof extends to infinite dimensional spaces the result valid for quasiperiodically forced linear differential equations and is based on Kuksin's estimate of solutions of homological equations with non-constant coefficients.