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    Dispersive estimates for the Schr\"{o}dinger equation with finite rank perturbations

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    In this paper, we investigate dispersive estimates for the time evolution of Hamiltonians H=βˆ’Ξ”+βˆ‘j=1NβŸ¨β‹…β€‰,Ο†jβŸ©Ο†j   in   Rd,  dβ‰₯1, H=-\Delta+\sum_{j=1}^N\langle\cdot\,, \varphi_j\rangle \varphi_j\quad\,\,\,\text{in}\,\,\,\mathbb{R}^d,\,\, d\ge 1, where each Ο†j\varphi_j satisfies certain smoothness and decay conditions. We show that, under a spectral assumption, there exists a constant C=C(N,d,Ο†1,…,Ο†N)>0C=C(N, d, \varphi_1,\ldots, \varphi_N)>0 such that βˆ₯eβˆ’itHβˆ₯L1βˆ’Lβˆžβ‰€Ctβˆ’d2,   for   t>0. \|e^{-itH}\|_{L^1-L^{\infty}}\leq C t^{-\frac{d}{2}}, \,\,\,\text{for}\,\,\, t>0. As far as we are aware, this seems to provide the first study of L1βˆ’L∞L^1-L^{\infty} estimates for finite rank perturbations of the Laplacian in any dimension. We first deal with rank one perturbations (N=1N=1). Then we turn to the general case. The new idea in our approach is to establish the Aronszajn-Krein type formula for finite rank perturbations. This allows us to reduce the analysis to the rank one case and solve the problem in a unified manner. Moreover, we show that in some specific situations, the constant C(N,d,Ο†1,…,Ο†N)C(N, d, \varphi_1,\ldots, \varphi_N) grows polynomially in NN. Finally, as an application, we are able to extend the results to N=∞N=\infty and deal with some trace class perturbations.Comment: 78 page
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