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arXiv 1502.02276math-phmath.MP
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径向Schr{<$}dinger算子在固定能量下的局部逆散射和Regge极点的局部化

Local inverse scattering at a fixed energy for radial Schr{ö}dinger operators and localization of the Regge poles

Thierry Daudé, Francois Nicoleau

摘要:

本文研究了$\R^n$,$n \geq 2$上径向薛定谔算子在固定能量下的逆散射问题。首先,我们考虑一类$\mathcal{A}$的潜力$q(r)$,它可以在$\Re z \geq 0$分析扩展,使$\mid q(z)\mid \leq C \ (1+ \mid z \mid )^{-ρ}$,$ρ\textgreater{} \frac{3}{2}$。如果$q$和$\tilde{q}$是两个这样的势,并且如果相应的相移$δ\_l$和$\tildeδ\_l$是超指数接近的,则$q=\tilde{q}$。其次,我们研究了一类可分解为$q(r)=q\_1(r) + q\_2(r)$的位势$q(r)$,使得$q\_1(r)$具有紧支集和$q\_2 (r) \in \mathcal{A}$。如果$q$和$\tilde{q}$是两个这样的潜力,我们表明,对于任何固定的$a\textgreater{}0$,${\ds{δ\_l - \tildeδ\_l \ = \ o \left( \frac{1}{l^{n-3}} \ \left( {\frac{ae}{2l}}\right)^{2l}\right)}}$当$l \rightarrow +\infty$当且仅当$q(r)=\tilde{q}(r)$几乎所有的$r \geq a$。这些证明在精神上与著名的Borg-Marchenko唯一性定理接近,并且严重依赖于Regge极点的局部化,Regge极点可以定义为复杂角动量平面中的共振。我们证明了对于非零的超指数下降势,Regge极点的个数总是无穷多,而且在右半平面上的任何垂直条中都不包含Regge极点.对于具有紧支集的势,我们能够明确地给出它们的渐近性。最后,对于在$\Re z \geq 0$中可以用$\mid q(z)\mid \leq C \ (1+ \mid z \mid )^{-ρ}$,$ρ\textgreater{}1$解析扩展的势,我们证明了Regge极点被限制在复平面上的一个垂直带中.

英文摘要:

We study inverse scattering problems at a fixed energy for radial Schrödinger operators on $\R^n$, $n \geq 2$. First, we consider the class $\mathcal{A}$ of potentials $q(r)$ which can be extended analytically in $\Re z \geq 0$ such that $\mid q(z)\mid \leq C \ (1+ \mid z \mid )^{-ρ}$, $ρ\textgreater{} \frac{3}{2}$. If $q$ and $\tilde{q}$ are two such potentials and if the corresponding phase shifts $δ\_l$ and $\tildeδ\_l$ are super-exponentially close, then $q=\tilde{q}$. Secondly, we study the class of potentials $q(r)$ which can be split into $q(r)=q\_1(r) + q\_2(r)$ such that $q\_1(r)$ has compact support and $q\_2 (r) \in \mathcal{A}$. If $q$ and $\tilde{q}$ are two such potentials, we show that for any fixed $a\textgreater{}0$, ${\ds{δ\_l - \tildeδ\_l \ = \ o \left( \frac{1}{l^{n-3}} \ \left( {\frac{ae}{2l}}\right)^{2l}\right)}}$ when $l \rightarrow +\infty$ if and only if $q(r)=\tilde{q}(r)$ for almost all $r \geq a$. The proofs are close in spirit with the celebrated Borg-Marchenko uniqueness theorem, and rely heavily on the localization of the Regge poles that could be defined as the resonances in the complexified angular momentum plane. We show that for a non-zero super-exponentially decreasing potential, the number of Regge poles is always infinite and moreover, the Regge poles are not contained in any vertical strip in the right-half plane. For potentials with compact support, we are able to give explicitly their asymptotics. At last, for potentials which can be extended analytically in $\Re z \geq 0$ with $\mid q(z)\mid \leq C \ (1+ \mid z \mid )^{-ρ}$, $ρ\textgreater{}1$ , we show that the Regge poles are confined in a vertical strip in the complex plane.

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