2002
DOI: 10.1007/s00041-002-0022-5
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On the Spectra of Elastostatic and Hydrostatic Layer Potentials on Curvilinear Polygons

Abstract: We give a complete description of the spectra of certain elastostatic and hydrostatic boundary layer potentials in L p , 1 < p < ∞, on bounded curvilinear polygons. In particular, our analysis shows that the spectral radii of these operators on L p , 2 ≤ p < ∞ are less than one. Such results are relevant in the context of constructively solving boundary value problems for the Lamé system of elasticity, the Stokes system of hydrostatics as well as the two dimensional Laplacian on curvilinear polygons. Our appro… Show more

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Cited by 28 publications
(36 citation statements)
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“…In contrast with the spectral properties of K : L p → L p [16], any non-essential point in the spectrum of K : H 1/2 → H 1/2 is an isolated eigenvalue of finite multiplicity (see Corollary 3.5), owing to the special symmetry features that K exhibits on H 1/2 . In modern computational applications involving K, or more general double layer potential operators such as those associated with the Helmholtz equation, such points in the discrete spectrum are easy to recognize.…”
Section: Introductionmentioning
confidence: 99%
“…In contrast with the spectral properties of K : L p → L p [16], any non-essential point in the spectrum of K : H 1/2 → H 1/2 is an isolated eigenvalue of finite multiplicity (see Corollary 3.5), owing to the special symmetry features that K exhibits on H 1/2 . In modern computational applications involving K, or more general double layer potential operators such as those associated with the Helmholtz equation, such points in the discrete spectrum are easy to recognize.…”
Section: Introductionmentioning
confidence: 99%
“…[36]. If p ≥ p 0 we can repeat the reasoning from the proof of Lemma 24 using results in [29], analogical to the result in [52], used in the proof.…”
Section: Medková I E O Tmentioning
confidence: 99%
“…We would like to point out that the case under consideration is both physically relevant and, from a technical standpoint, the most challenging among all Neumann-type boundary problems for the system of elastostatics. Indeed, the spectral analysis of K undertaken here is considerably more difficult and subtle than the one for the layer potential operator associated with the pseudo-stress conormal derivative, considered previously in [17,18].…”
Section: Introductionmentioning
confidence: 98%