2016/02/15 by Mikhail Belishev, Belishev, Mikhail, Aleksei Vakulenko +1
Mathematics · Physics and Astronomy · #35L51 #35Qxx #35R30 #Analysis of PDEs (math.AP) #F.2.2 #FOS: Mathematics #FOS: Physical sciences #I.2.7 #Mathematical Physics (math-ph) #acm:35L51 #acm:35Qxx #acm:35R30 #math-ph #math.AP #math.MP #msc:35L51 #msc:35Qxx #msc:35R30
paper · pdf · doi:10.48550/arxiv.1602.05066
33 pages, 1 figure
arxiv created 2016/02/15 · arxiv updated 2016/02/17
We deal with a dynamical system utt-Δu+qu=0 & \rm in Ω× (0,T)
u|t=0=ut|t=0=0 & \rm in Ω
∂νu = f & \rm in ∂Ω× [0,T] , where Ω⊂ \mathbb Rn is a bounded domain, q ∈ L_∞(Ω) a real-valued function, ν the outward normal to ∂ Ω, u=uf(x,t) a solution. The input/output correspondence is realized by a response operator RT: f ↦ uf|∂Ω× [0,T] and its relevant extension by hyperbolicity R2T. Ope\-rator R2T is determined by q|ΩT, where ΩT:=\x ∈ Ω | \rm dist (x,∂ Ω)<T\. The inverse problem is: Given R2T to recover q in ΩT. We solve this problem by the boundary control method and describe the \it ne\-ces\-sary and sufficient conditions on R2T, which provide its solvability.