2000
DOI: 10.1090/trans2/199/04
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Spectral problems in singularly perturbed domains and selfadjoint extensions of differential operators

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Cited by 30 publications
(33 citation statements)
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“…The known results are given in particular for singular perturbations of isolated points of the boundary (small holes in the domain, see [14], [15], [5], [1], [13], [35] and others), perturbations of straight boundaries including perturbations by changing the type of boundary conditions (cf. [2]- [3]), and the dependence of the obtained results in more general geometrical domains on the curvature is clarified in [8,22,23] in the case of scalar equations.…”
Section: Asymptotic Analysis Of Eigenvalues In Singularly Perturbed Dmentioning
confidence: 99%
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“…The known results are given in particular for singular perturbations of isolated points of the boundary (small holes in the domain, see [14], [15], [5], [1], [13], [35] and others), perturbations of straight boundaries including perturbations by changing the type of boundary conditions (cf. [2]- [3]), and the dependence of the obtained results in more general geometrical domains on the curvature is clarified in [8,22,23] in the case of scalar equations.…”
Section: Asymptotic Analysis Of Eigenvalues In Singularly Perturbed Dmentioning
confidence: 99%
“…The coefficients M j kp in (25) form the (6 × 6)-matrix M j which is called the polarization matrix of the elastic inclusion ω j (see [28,41] and also [[20]; Ch. 6], [5], [21]). Some properties of the polarization matrix, and some comments on the solvability of problem (23) are given in section 4.…”
Section: Formal Construction Of Asymptoticsmentioning
confidence: 99%
“…We consider the functional r Asymptotic structures for specific problems with the logarithmic growth of fundamental solutions, turn out to be quite complex and therefore, of limited practical interest for analysis of functional (9). The main particularity of the asymptotic analysis, beside the presence of boundary layers near the arcs yk, ..., ^(hI, is the form of asymptotic terms which are rational functions of the large parameter I In hl.…”
mentioning
confidence: 99%
“…On the other hand, the proposed singularities are not included in the energy class H 1 however the resulting singular solutions are still in the space L q ( 0 ) , for q 2 I. The main profit from our point of view for such modeling is the possibility, with the singular solutions, for asymptotically exact approximation of functional (9), under the condition that for some q E [I, CQ) and for any u, v E ~~( 0 )~ the following inequality is valid with the constant CF independent of h E (0, ho] and u, v. Modeling defects in media by an application of extensions of differential operators which give rise to the singular solutions comes back to the work [3] and is developped in [20], [16], [MI, [17], [9] and in other publications, for problems of mathematical physics and general elliptic systems. There are two possibilities for realization of such ideas.…”
mentioning
confidence: 99%
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