GLOBAL UNIQUENESS AND STABILITY IN DETERMINING COEFFICIENTS OF WAVE EQUATIONS
By Oleg Yu. Imanuvilov, Masahiro Yamamoto. 2001
196 citations recorded by the source corpus.
Subfields: Computational Theory and Mathematics, Mathematical Physics, Mechanics of Materials
View Paper: https://www.semanticscholar.org/paper/7e957d985ce88f460c8178209ec2d35416449470
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In Computational Theory and Mathematics
- Masahiro Yamamoto
- Michael V. Klibanov
- Sylvain Ervedoza
- Mourad Bellassoued *
- D. Jellali
- Lucie Baudouin
- Oleg Yu. Imanuvilov
- Maya de Buhan
In Mathematical Physics
- Masahiro Yamamoto
- Michael V. Klibanov
- Sylvain Ervedoza
- Mourad Bellassoued *
- D. Jellali
- Oleg Yu. Imanuvilov
- Jean-Pierre Puel
- Lucie Baudouin
In Mechanics of Materials
- Masahiro Yamamoto
- Mourad Bellassoued *
- D. Jellali
- Michael V. Klibanov
- Lucie Baudouin
- Oleg Yu. Imanuvilov
- Sylvain Ervedoza
- Maya de Buhan
Citations in the corpus
- Inverse source problem for the hyperbolic equation with a time-dependent principal part (2015, unknown): “Motivated by the global Lipschitz stability obtained in [13,14] for the inverse source problem for wave equations, in this paper we investigate the same problem for the general hyperbolic equation with time-dependent principal part.”
- Uniqueness and stability in determining the speed of propagation of second-order hyperbolic equation with variable coefficients (2004, unknown): “For suitable ! and T>0, Immanuvilov and Yamamoto’s result [7] gives an stability estimate of Hölder type.”
- Uniqueness and stability in an inverse problem for the Schrödinger equation (2007, background): “They are related to the same kind of inverse problems of determining a potential, some of them ([10], [13]) with a Dirichlet boundary data and a Neumann measurement and others with a Neumann boundary data and a Dirichlet measurement ([5], [6]).”
- Carleman estimates for the non-stationary Lamé system and the application to an inverse problem (2005, result): “As for the corresponding results on the stability for inverse problems for scalar hyperbolic equations, we refer to [22–24] for example.”
- An inverse problem for the dynamical Lamé system with two sets of boundary data (2003, unknown): “4 Proof of Main Theorem 2.1 We will combine the method of Bukhgeim and Klibanov [3], its modification by Imanuvilov and Yamamoto [12], and the Carleman estimate (3.1) for the elasticity system.”
- Stability estimate for the hyperbolic inverse boundary value problem by local Dirichlet-to-Neumann map (2008, methodology): “In order to extend the estimate on the conic subset to an estimate on the ball, we use an idea of Heck and Wang [10] and conditional stability for analytic continuation established by Vessella [32].”
- Lipschitz stability for a hyperbolic inverse problem by finite local boundary data (2006, methodology): “A Carleman estimate was first applied to inverse problems by Bukhgeim and Klibanov [3], and see also [2,10,15,16].”
- Carleman estimates for parabolic equations and applications (2009, methodology): “Yamamoto and Zou [143] proved the Lipschitz stability in determining c(x), x ∈ and for it, the assumption u(x, t0) > 0 for x ∈ is essential.”
- The seismic reflection inverse problem (2009, background): “For example, recent years have seen a flowering of work on inverse problems for wave equations from the purely mathematical point of view—see for example Belishev (2007), Stefanov and Uhlmann (2005), Imanuvilov and Yamamoto (2001).”
- Global uniqueness for a coefficient inverse problem for the non-stationary transport equation via Carleman estimate (2008, background): “A variety of works with uniqueness and stability results for coefficient inverse problems w ere published, which are based on the idea of [4] and [13]-[15], see, for example, Bellassoued [2], [3], Imanuvilov and Yamamoto [9], [ 10 ] and [11] for the case of hyperbolic equations.”
- Global Carleman Estimates for Waves and Applications (2011, methodology): “We will first prove Carleman estimates similar to the ones of Theorems 1.1–1.2 for the operator , corresponding to a potential equal to zero.”