English

Inverse scattering with the data at fixed energy and fixed incident direction

Mathematical Physics 2013-02-21 v1 math.MP

Abstract

Consider the Schr\"odinger operator 2+q-\nabla^2+q q,, q=q(x), x \in \mathbf{R}^3.Let. Let A(\beta,\alpha, k)bethecorrespondingscatteringamplitude, be the corresponding scattering amplitude, k^2betheenergy, be the energy, \alpha \in S^2betheincidentdirection, be the incident direction, \beta \in S^2bethedirectionofscatteredwave, be the direction of scattered wave, S^2betheunitspherein be the unit sphere in \mathbf{R}^3.Assumethat. Assume that k=k_0 >0isfixed,and is fixed, and \alpha=\alpha_0isfixed.Thenthescatteringdataare is fixed. Then the scattering data are A(\beta)= A(\beta,\alpha_0, k_0)=A_q(\beta)isafunctionon is a function on S^2.Thefollowinginvers. The following invers \textit{IP: Given an arbitrary fL2(S2)f \in L^2(S^2) and an arbitrary small number qC0(D)q \in C_0^{\infty}(D), where DR3D \in \mathbf{R}^3 is an arbitrary fixed domai ||A_q(\beta)-f(\beta)||_{L^2(S^2)} < \epsilon?} A positive answer to this question is given. A method for constructing such a qisproposed.Thereareinfinitelymanysuch is proposed. There are infinitely many such q$, not necessarily real-valued.

Keywords

Cite

@article{arxiv.1302.5000,
  title  = {Inverse scattering with the data at fixed energy and fixed incident direction},
  author = {A. G. Ramm},
  journal= {arXiv preprint arXiv:1302.5000},
  year   = {2013}
}
R2 v1 2026-06-21T23:29:30.900Z