2017
DOI: 10.1016/j.matpur.2016.11.001
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Stabilization of the wave equation with Ventcel boundary condition

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Cited by 26 publications
(22 citation statements)
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“…The starting point is boundary Carleman estimates for the operator −∆ − k 2 , k ≥ 1, for functions u satisfying the Robin boundary conditions (∂ ν − ik)u = 0 on ∂Ω. Such Carleman estimates are essentially well known and are discussed in Section 2, following the works by Fursikov-Imanuvilov [19], Lebeau-Robbiano [39], [40], Burq [10], and Buffe [8], see also [37] and [38]. Let us mention that the presence of the large parameter k in the boundary conditions makes the situation more complicated and in addition to 1/k, it becomes natural to introduce a second small parameter h such that 0 < h ≪ 1/k.…”
Section: Remarkmentioning
confidence: 99%
“…The starting point is boundary Carleman estimates for the operator −∆ − k 2 , k ≥ 1, for functions u satisfying the Robin boundary conditions (∂ ν − ik)u = 0 on ∂Ω. Such Carleman estimates are essentially well known and are discussed in Section 2, following the works by Fursikov-Imanuvilov [19], Lebeau-Robbiano [39], [40], Burq [10], and Buffe [8], see also [37] and [38]. Let us mention that the presence of the large parameter k in the boundary conditions makes the situation more complicated and in addition to 1/k, it becomes natural to introduce a second small parameter h such that 0 < h ≪ 1/k.…”
Section: Remarkmentioning
confidence: 99%
“…For the estimate of U 2 , we note that it satisfies a Ventcel boundary condition on J 1 and the Dirichlet boundary condition on J 0 . Hence, we use the following result, which is basically a consequence of a Carleman estimate obtained in [11]. However for the sake of completeness, we prove the next result in Appendix A.…”
Section: Estimates On the Velocitymentioning
confidence: 88%
“…Optimizing this inequality with respect to τ τ 4 (see, for instance, [11,Lemma 8.4]) allows us to conclude the proof of Theorem 5.3.…”
Section: Patching the Estimates Togethermentioning
confidence: 99%
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