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2016
DOI: 10.2140/apde.2016.9.1259
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On the negative spectrum of the Robin Laplacian in corner domains

Abstract: For a bounded corner domain $\Omega$, we consider the Robin Laplacian in $\Omega$ with large Robin parameter. Exploiting multiscale analysis and a recursive procedure, we have a precise description of the mechanism giving the ground state of the spectrum. It allows also the study of the bottom of the essential spectrum on the associated tangent structures given by cones. Then we obtain the asymptotic behavior of the principal eigenvalue for this singular limit in any dimension, with remainder estimates. The sa… Show more

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Cited by 26 publications
(45 citation statements)
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References 31 publications
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“…Schrödinger operators with singular potential, modeled by δinteractions supported on smooth cones, are investigated in [4,25] whereas the case of the Laplacian with Robin boundary conditions in smooth conical domains is dealt with in [8,30]. Finally, for problems related with polyhedral geometries, let us mention [7] where the magnetic Laplacian in three-dimensional corner domains is studied as well as [9] where the bottom of the essential spectrum of the Robin Laplacian is characterized for polyhedral cones.…”
Section: Introduction and Main Resultsmentioning
confidence: 99%
“…Schrödinger operators with singular potential, modeled by δinteractions supported on smooth cones, are investigated in [4,25] whereas the case of the Laplacian with Robin boundary conditions in smooth conical domains is dealt with in [8,30]. Finally, for problems related with polyhedral geometries, let us mention [7] where the magnetic Laplacian in three-dimensional corner domains is studied as well as [9] where the bottom of the essential spectrum of the Robin Laplacian is characterized for polyhedral cones.…”
Section: Introduction and Main Resultsmentioning
confidence: 99%
“…Denote q := p p−1 the Hölder conjugate of p. In this note we prove the following result: Theorem 1. As α tends to +∞ there holds (1) Λ(α) = (1 − p)α q + o(α q ).…”
Section: Introductionmentioning
confidence: 99%
“…It seems that the asymptotic behavior for large α was first addressed by Lacey, Ockedon and Sabina [8] for the linear situation (p = 2), and C 1 domains represent a borderline case. On one hand, the asymptotic behavior (1) is not valid for non-smooth domains [1,6,9]. On the other hand, for C 1,1 domains one has Λ(α) = (1 − p)α q − Hα + o(α) with H being the maximum mean curvature of the boundary [7], which is much more detailed, but the proof depends heavily on the existence of a tubular neighborhood of the boundary and on the regularity of boundary curvatures.…”
Section: Introductionmentioning
confidence: 99%
“…On the other hand, only partial results are available for domains with a non-smooth boundary, cf. [8,23,32].…”
Section: Introductionmentioning
confidence: 99%