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On the modified scattering of $3$-d Hartree type fractional Schrödinger equations with Coulomb potential

Published 23 Oct 2017 in math.AP | (1710.08552v1)

Abstract: In this paper we study 3-d Hartree type fractional Schr\"odin-ger equations: \begin{equation} i\partial_{t}u-|\nabla|{\alpha}u = \lambda\left(|x|{-\gamma} *| u|{2} \right)u,\;\;1 < \alpha < 2,\;\;0 < \gamma < 3,\;\; \lambda \in \mathbb R \setminus {0}. \end{equation} In \cite{cho} it is known that no scattering occurs in L<sup>2L<sup>2 for the long range ($0 &lt; \gamma \le 1$). In \cite{c0, chooz2, cho1} the short-range scattering ($1 &lt; \gamma &lt; 3$) was treated for the scattering in H<sup>sH<sup>s. In this paper we consider the critical case (γ=1\gamma = 1) and prove a modified scattering in L<sup>L<sup>\infty on the frequency to the Cauchy problem with small initial data. For this purpose we investigate the global behavior of xe<sup>it</sup>ux e<sup>{it\nabla}</sup> u, x<sup>2</sup>e<sup>it</sup>ux<sup>2</sup> e<sup>{it\nabla}</sup> u and ξ<sup>5</sup>e<sup>it</sup>u^\langle\xi\rangle<sup>5</sup> \widehat{e<sup>{it\nabla}</sup> u}. Due to the non-smoothness of \nabla near zero frequency the range of α\alpha is restricted to (1710,2)(\frac{17}{10}, 2).

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