2015
DOI: 10.1007/978-3-319-12577-0_21
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Viewing the Steklov Eigenvalues of the Laplace Operator as Critical Neumann Eigenvalues

Abstract: We consider the Steklov eigenvalues of the Laplace operator as limiting Neumann eigenvalues in a problem of boundary mass concentration. We discuss the asymptotic behavior of the Neumann eigenvalues in a ball and we deduce that the Steklov eigenvalues minimize the Neumann eigenvalues. Moreover, we study the dependence of the eigenvalues of the Steklov problem upon perturbation of the mass density and show that the Steklov eigenvalues violates a maximum principle in spectral optimization problems.

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Cited by 30 publications
(39 citation statements)
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“…Using a mass perturbation argument, they prove that the Steklov problem can in fact be viewed as a limiting Neumann problem where the mass is distributed only on the boundary. Note that this construction was already performed in [19] for the Laplace operator, obtaining similar results (see also [16,20] for the computation of the topological derivative). Moreover, this justifies the fact of thinking of Steklov problems in terms of vibrating objects (plates or membranes) where the mass lies only on the boundary (see [23]).…”
Section: Introductionmentioning
confidence: 56%
“…Using a mass perturbation argument, they prove that the Steklov problem can in fact be viewed as a limiting Neumann problem where the mass is distributed only on the boundary. Note that this construction was already performed in [19] for the Laplace operator, obtaining similar results (see also [16,20] for the computation of the topological derivative). Moreover, this justifies the fact of thinking of Steklov problems in terms of vibrating objects (plates or membranes) where the mass lies only on the boundary (see [23]).…”
Section: Introductionmentioning
confidence: 56%
“…We refer e.g., to [9] for a more detailed discussion on the Steklov eigenvalue problem for the biharmonic operator. We have the following theorem: We refer to [33,34] for the proof of Theorem 4.18 in the case of the Laplace operator and to [9] for the proof of Theorem 4.18 in the case of the biharmonic operator, and for more information on the convergence of Neumann eigenvalues to Steklov eigenvalues via mass concentration to the boundary. We remark that the proof of Theorem 4.18 for all values of m ∈ N follows exactly the same lines as the proof of the case m = 1 and m = 2.…”
Section: 3mentioning
confidence: 99%
“…However, instead of studying each eigenvalue problem individually, it is also interesting to explore relationships and inequalities between eigenvalues of different eigenvalue problems. Among this type of results, one can mention the relationships between the Laplace and Steklov eigenvalues studied in [21,11,18], and various inequalities between the first nonzero eigenvalue of problems (1.2)-(1.5) on bounded domains of R 2 obtained by Kuttler and Sigilito in [10]; see Table 1 (Note that there was a misprint in Inequality VI in [10]. The correct version of the inequality is stated in Table 1.).…”
Section: Introductionmentioning
confidence: 99%