Inverse Problems · 1987 · 53 citations · 2 references
Natural SciencesMathematicsDifferential EquationsFinite Element AnalysisTheoretical PhysicsBoundary ConditionsIntegral EquationsPartial Differential EquationsScattering ProblemsScattering TheoryUniqueness TheoryInverse ScatteringScattering Inverse ProblemsUniqueness In Elliptic EquationsUniqueness In Inverse ProblemsUniqueness Of SolutionsUniqueness TheoremsUniqueness Theorems For Partial Differential Equations
Let N=(u:( Del 2+k2)u=0), N1=( psi :( Del 2+k2-q(x)) psi =0) in D contained in/implied by R3, where D is a bounded domain, k=constant >0, q(x) in Linfinity (D). Suppose that f in LP(D), p>or=1, and integral fu psi dx=0 for all u in N and psi in N1. Then f=0. Results of this type are used to prove uniqueness theorems in inverse scattering. In particular, the author proves that the scattering amplitude A( theta ', theta ,k) known at a fixed k>0 for all theta ', theta in S2 determines the compactly supported potential q(x) uniquely. He also proves that the surface data u(x,y,k), For all x, y in P=(x:x3=0) at a fixed k>0 determine the compactly supported nu (x) in L2(D) uniquely. Here ( Del 2+k2+k2 nu (x))=- delta (x-y) in R3, D contained in/implied by R-3=(x:x3<0) is a bounded domain.
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