English

On Characterization of Inverse Data in the Boundary Control Method

Analysis of PDEs 2016-02-17 v1 Mathematical Physics math.MP

Abstract

We deal with a dynamical system \begin{align*} & u_{tt}-\Delta u+qu=0 && {\rm in}\,\,\,\Omega \times (0,T)\\ & u\big|_{t=0}=u_t\big|_{t=0}=0 && {\rm in}\,\,\,\overline \Omega\\ & \partial_\nu u = f && {\rm in}\,\,\,\partial\Omega \times [0,T]\,, \end{align*} where ΩRn\Omega \subset {\mathbb R}^n is a bounded domain, qL(Ω)q \in L_\infty(\Omega) a real-valued function, ν\nu the outward normal to Ω\partial \Omega, u=uf(x,t)u=u^f(x,t) a solution. The input/output correspondence is realized by a response operator RT:fufΩ×[0,T]R^T: f \mapsto u^f\big|_{\partial\Omega \times [0,T]} and its relevant extension by hyperbolicity R2TR^{2T}. Ope\-rator R2TR^{2T} is determined by qΩTq\big|_{\Omega^T}, where ΩT:={xΩdist(x,Ω)<T}\Omega^T:=\{x \in \Omega\,|\,\,{\rm dist\,}(x,\partial \Omega)<T\}. The inverse problem is: Given R2TR^{2T} to recover qq in ΩT\Omega^T. We solve this problem by the boundary control method and describe the {\it ne\-ces\-sary and sufficient} conditions on R2TR^{2T}, which provide its solvability.

Keywords

Cite

@article{arxiv.1602.05066,
  title  = {On Characterization of Inverse Data in the Boundary Control Method},
  author = {Mikhail Belishev and Aleksei Vakulenko},
  journal= {arXiv preprint arXiv:1602.05066},
  year   = {2016}
}

Comments

33 pages, 1 figure

R2 v1 2026-06-22T12:51:24.173Z