2004
DOI: 10.1017/s0956792504005649
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A uniqueness result in an inverse hyperbolic problem with analyticity

Abstract: Link to this article: http://journals.cambridge.org/abstract_S0956792504005649 How to cite this article: YU. E. ANIKONOV, J. CHENG and M. YAMAMOTO (2004). A uniqueness result in an inverse hyperbolic problem with analyticity.We prove the uniqueness for the inverse problem of determining a coefficient q(x ∈ R n and t > 0, from observations of u| Γ ×(0,T ) and the normal derivative ∂u ∂ν | Γ ×(0,T ) where Γ is an arbitrary C ∞ -hypersurface. Our main result asserts the uniqueness of q over R n provided that T > … Show more

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Cited by 9 publications
(13 citation statements)
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“…Now we multiply (27) by v(t, x) ∈ H 1 (Q) and integrate over Q. We get, after integrating by parts, taking into account the following: u| Σ = 0, u(T, x) = 0, ∂ ν u| G = 0, u| t=0 = ∂ t u| t=0 = 0 and A (1) is compactly supported in Q:…”
Section: Integral Identitymentioning
confidence: 99%
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“…Now we multiply (27) by v(t, x) ∈ H 1 (Q) and integrate over Q. We get, after integrating by parts, taking into account the following: u| Σ = 0, u(T, x) = 0, ∂ ν u| G = 0, u| t=0 = ∂ t u| t=0 = 0 and A (1) is compactly supported in Q:…”
Section: Integral Identitymentioning
confidence: 99%
“…Later it was developed by Belishev, Kurylev, Katchalov, Lassas, Eskin and others; see [17] and references therein. Eskin in [10,12] developed a new approach based on the BC method for determining the time-independent vector and scalar potentials assuming A 0 = 0 in (1). Hyperbolic inverse problems for time-independent coefficients have been extensively studied by Yamamoto and his collaborators as well; see [1,2,8,13,14].…”
Section: Introductionmentioning
confidence: 99%
“…Hence, by assuming that ∇ • J = 0, we may eliminate a class of non-radiating sources in order to ensure the uniqueness of IP1. Moreover, even though (1.2) can be reduced into a simple vector wave equation under the divergence free condition, we may not use the results in [6] and [23] for the hyperbolic wave equation and Helmholtz equation directly. The reason is that for the Maxwell equation, it is more practical to use the tangential trace of the electric field E(x, t) × ν on the boundary Γ R as a data rather than the total field E(x, t) on the boundary Γ R .…”
Section: Ip1: Determination Of the Spatial Functionmentioning
confidence: 99%
“…In this work, we consider directly how to determine the temporal and spatial source functions for the time-dependent Maxwell equations. We refer to [6,25,34,26,22] for the method of applying Carleman estimates to inverse source problems for hyperbolic systems, and to [32,31] for other formulation of inverse problems which are related to Maxwell's equations. Our approach of converting the time-dependent problem into a multi-frequency problem in the frequency domain seems natural.…”
mentioning
confidence: 99%
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