2012
DOI: 10.1007/s00220-012-1431-1
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Inverse Problems With Partial Data for a Magnetic Schrödinger Operator in an Infinite Slab and on a Bounded Domain

Abstract: In this paper we study inverse boundary value problems with partial data for the magnetic Schrödinger operator. In the case of an infinite slab in R n , n ≥ 3, we establish that the magnetic field and the electric potential can be determined uniquely, when the Dirichlet and Neumann data are given either on the different boundary hyperplanes of the slab or on the same hyperplane. This is a generalization of the results of Li and Uhlmann (Inverse Probl Imaging 4(3):449-462, 2010), obtained for the Schrödinger op… Show more

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Cited by 44 publications
(93 citation statements)
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“…First, Theorem 1.1 is stated in a general unbounded domain subject only to condition (1.1). This makes an important difference with other related results which, to our best knowledge, have all been stated in specific unbounded domains like a slab, the half space or a cylindrical domain (see [33,37,14,15]). In particular, Theorem 1.1 holds true with domains having different types of geometrical deformations like bends or twisting, which are frequently used in problems of transmission for improving the propagation.…”
Section: Comments About Our Resultsmentioning
confidence: 82%
“…First, Theorem 1.1 is stated in a general unbounded domain subject only to condition (1.1). This makes an important difference with other related results which, to our best knowledge, have all been stated in specific unbounded domains like a slab, the half space or a cylindrical domain (see [33,37,14,15]). In particular, Theorem 1.1 holds true with domains having different types of geometrical deformations like bends or twisting, which are frequently used in problems of transmission for improving the propagation.…”
Section: Comments About Our Resultsmentioning
confidence: 82%
“…Unique determination of a compactly supported electric potential of the Laplace equation in an infinite slab, by partial DN map, is established in . This result was extended to the magnetic case in and to bi‐harmonic operators in .…”
Section: Introductionmentioning
confidence: 89%
“…Since γ 0 is tangent to ∂ M at x 0 , we have τ x n (x 0 ) = 0 by (117). The third term in the l.h.s.…”
Section: Sketch Of the Proof Of Theorem 228mentioning
confidence: 96%
“…The case of partial data on a slab was studied in [122]. The DN map with partial data for the magnetic Schrödinger operator was studied in [51,109,117,198]. The case of the polyharmonic operator was considered in [118].…”
Section: The Uniqueness Proofmentioning
confidence: 99%