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3rd International ISAAC Congress
August 20-25, 2001
Freie Universitaet Berlin
Berlin, Germany

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Inverse-Scattering with the time-dependent and time-independent Schroedinger equation
by
Swanhild Bernstein
Bauhaus-Universitaet Weimar, Institute of Mathematics and Physics, 99421 Weimar, Germany

We discuss I.S.T. (Inverse Scattering Transform) schemes for multidimensional equations. The application of the [`(\partial)] method to study nonlinear evolution equations in two spatial dimensions has led to the development of a general formalism to implement inverse scattering in n spatial dimensions by M.J. Ablowitz and A.I. Nachman.
We discuss inverse scattering associated with the Schrödinger-type equation
\sigma  \partialv

\partialy
+ n
å
j=1 
 \partial2 v

\partialxj2
+u(
-->
x
 
, y)v = 0,
with \sigma = \sigmar+i\sigmaI,  [x\vec]=(x1, x2, ... , xn) in Rn,  y in R. It turns out that there is a very important constraint which the scattering data must satisfy. The inverse scattering problem consists in determining the potential u([x\vec], y) from the inverse data T([k\vec]R, [k\vec]I, [(\xi)\vec]). However, it is immediatly obvious that there is a serious redundancy question. Namely T([k\vec]R, [k\vec]I, [(\xi)\vec]) is a function of 3n parameters with one restriction, i.e. T will be given as a function of 3n-1 variables and we widh to construct a function u([x\vec], y) depending on n+1 variables. There are several possible reconstruction formulae for u([x\vec], y). However, crucial restrictions on T are imposed by the requirement that u depends only on [x\vec],  y and decays at \infty. This is part of the characterization question: i.e. which inverse data T([k\vec]R, [k\vec]I, [(\xi)\vec]) are ädmissible". We will use a Borel-Pompeiu formula in Cn to construct admissible data and use the fact that holomorphic functions are complex monogenic functions. In this way we will need no so-called "miracle condition" or any similar requirement on the inverse data T([k\vec]R, [k\vec]I, [(\xi)\vec]).
We will apply our method to the time-dependent and the time-independent Schrödinger equation which are special cases of the general one.

Date received: July 4, 2001


Copyright © 2001 by the author(s). The author(s) of this document and the organizers of the conference have granted their consent to include this abstract in Atlas Conferences Inc. Document # cahv-54.