It has been known for some time that solutions of linear Schrödinger operators on the torus, with bounded, smooth, time dependent (order zero pseudo-differential) potential, have Sobolev norms growing at most like t when t → +∞ for any > 0. This property is proved exploiting the fact that, on the circle, successive eigenvalues of the laplacian are separated by increasing gaps (and a more involved, but similar property, for clusters of eigenvalues in higher dimension). We study here the case of solutions ofwhere V is a time periodic pseudo-differential order zero perturbation. In this case, the gap between successive eigenvalues of the stationary operator is constant. We show that there are order zero potentials V for which some solutions u have Sobolev norms of order s growing like t s/2 when t → +∞, i.e. lim infThe idea of the proof is to construct a potential which, at the classical level, pulls frequencies to higher modes, so that they will be of size √ t at time t. One contructs then the wanted solution passing from the classical level to the quantum one.
IntroductionLet P 0 be an elliptic self-adjoint differential operator of positive order on some Riemannian manifold M . Consider t → V (t) a smooth family of self-adjoint operators on M , or order zero, and the Schrödinger equationDenote by H s the Sobolev space associated to P 0 , defined when s is an even integer 2kWe are interested in estimating u(t, ·) H s when t goes to infinity. If V is time independent, it is immediate that u(t, ·) H s = u(0, ·) H s . Over the last fifteen years, several results have been obtained by different authors for time dependent potentials V , under convenient spectral assumptions on P 0 and V . Our aim is to This work was partially supported by the ANR project Equa-disp.