In this paper I prove a L p &L p estimate for the solutions to the one-dimensional Schro dinger equation with a potential in L 1 # where in the generic case #>3Â2 and in the exceptional case (i.e., when there is a half-bound state of zero energy) #>5Â2. I use this estimate to construct the scatterin
On Inverse Scattering for theN-Body Schrödinger Equation
✍ Scribed by Roman G Novikov
- Publisher
- Elsevier Science
- Year
- 1998
- Tongue
- English
- Weight
- 639 KB
- Volume
- 159
- Category
- Article
- ISSN
- 0022-1236
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✦ Synopsis
We consider the generalized N-body Schro dinger operator H=&2+q(x), q(x)= :
with short-range regular interactions. We obtain, in particular, the following results.
(1) We give new formulas and proofs relating high energy asymptotics (in a weak sense) of the scattering operators S ;: (with the same cluster decomposition a for : and ;) and the X-ray transform PI ;: (defined on the set of all lines in X a with nonsingular directions) of the effective potentials I ;: (x a ), x a # X a . These results significantly clarify some of those given in the literature.
(2) We describe completely Ker P and give a method for reconstruction of I ;: (mod Ker P) from PI ;: .
(3) We prove pointwise high energy asymptotics for the two-cluster-twocluster scattering amplitudes f ;: with the Fourier transform I ;: in the leading term (for the case when the cluster decomposition for : and ; is the same).
(4) We give several additional results for the case (of perturbed stratified medium) when q(x)=v a (x a )+v b (x b ), x a =x 1 , x b =(x 1 , ..., x d )=x and each v c (x c ) rapidly decreases as |x c | Ä , c=a, b.
Our results (including proofs) in some cases significantly simplify methods of high energy inverse scattering for the N-body Schro dinger operator given earlier by Wang and by Enss and Weder. 1998 Academic Press 0. INTRODUCTION The studies of the inverse scattering problem for the N-body Schro dinger equation, which use results of the modern direct scattering theory for this equation, were started in [W2] (and subsequent works [W4, W5]), [EW2] (and subsequent works [EW3, EW4]), [N1] (and subsequent work [N2]), [V].
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