2013
DOI: 10.1080/17415977.2013.827181
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An alternating iterative procedure for the Cauchy problem for the Helmholtz equation

Abstract: We present a modification of the alternating iterative method, which was introduced by Kozlov and Maz'ya, for solving the Cauchy problem for the Helmholtz equation in a Lipschitz domain. The reason for this modification is that the standard alternating iterative algorithm does not always converge for the Cauchy problem for the Helmholtz equation. The method is then implemented numerically using the finite difference method.

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Cited by 38 publications
(39 citation statements)
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“…This method has gained a lot of popularity since then. In this regard, we also mention the work of Avdonin, Kozlov and Maxwell [2] for a nonlinear elliptic equation and the work of Berntsson, Kozlov, Mpinganzima and Turesson [14] for the Helmholtz equation. Andrieux, Baranger and Ben Abda [1] have improved in some sense the algorithm of [58].…”
Section: Introductionmentioning
confidence: 99%
“…This method has gained a lot of popularity since then. In this regard, we also mention the work of Avdonin, Kozlov and Maxwell [2] for a nonlinear elliptic equation and the work of Berntsson, Kozlov, Mpinganzima and Turesson [14] for the Helmholtz equation. Andrieux, Baranger and Ben Abda [1] have improved in some sense the algorithm of [58].…”
Section: Introductionmentioning
confidence: 99%
“…Let us finally prove that the operator A is non-expansive. If Ψ D ∈ Λ, the sequence (||u k || α,η ) k is decreasing; see [17,18]. We then obtain ||AΨ D || 0,ΓI = ||u 2 || α,η ≤ ||u 0 || α,η = ||Ψ D || 0,ΓI .…”
Section: The Optimized Dirichlet-order 2 Alternating Methodsmentioning
confidence: 99%
“…In fact, this procedure, which extends analogue results for elasticity problems (see [14,15]), has become very popular lately, especially in the context of obstacle detection [16], or coefficient reconstruction [3]. The alternating method has been applied successfully to the Cauchy Stokes problem and similar problems, see, for example [17,18,19]. A deep one tool relates the two approaches.…”
Section: Introductionmentioning
confidence: 99%
“…Similarly, by definition, ( , ) = ( 0 , 2 ), and using the normal bending moment boundary condition for 2 on Γ 1 together with (13) and the symmetry of the bilinear form (⋅, ⋅),…”
Section: The Adjoint Of the Operatormentioning
confidence: 99%