Abstract

We construct two-term asymptotics $$\lambda ^\varepsilon _k= \varepsilon ^{m-2}(M+\varepsilon \mu _k+ O(\varepsilon ^{3/2}) )$$ of eigenvalues of a mixed boundary-value problem in $$\Omega \subset {{\mathbb {R}}}^2$$ with many heavy ( $$m>2$$ ) concentrated masses near a straight part $$\Gamma $$ of the boundary $$\partial \Omega $$ . $$\varepsilon $$ is a small positive parameter related to size and periodicity of the masses; $$k\in {\mathbb N}$$ . The main term $$M>0$$ is common for all eigenvalues but the correction terms $$\mu _k$$ , which are eigenvalues of a limit problem with the spectral Steklov boundary conditions on $$\Gamma $$ , exhibit the effect of asymptotic splitting in the eigenvalue sequence enabling the detection of asymptotic forms of eigenfunctions. The justification scheme implies isolating and purifying singularities of eigenfunctions and leads to a new spectral problem in weighed spaces with a “strongly” singular weight.

Highlights

  • Introduction and setting of the problemIn this paper we introduce unaccustomed splitting asymptotic procedure for eigenvalues, purifying singularities of eigenfunctions

  • The spectral problem under consideration is a mixed boundary value problem for the Laplace operator in a domain Ω ⊂ R2 with heavy concentrated masses periodically distributed along a straight part Γ of the boundary

  • We construct the two-term asymptotics, that is, the main term and the first correction term, which gives a much more precise information on the behavior of the eigenvalues as ε → 0+ and allows us to describe the asymptotic structure of the corresponding eigenfunctions which exhibit a strongly oscillatory character

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Summary

Introduction and setting of the problem

In this paper we introduce unaccustomed splitting asymptotic procedure for eigenvalues, purifying singularities of eigenfunctions. The density of the concentrated masses is of order ε−m, with m > 2, and the period is ε ≪ 1. This problem has remained unsolved for a long time and has led to results that are currently the subject of discussion (cf Remark 1.1 and Section 1.3). We claim that all the results and proofs that we present are necessary to show the approach of the eigenvalues, and of the eigenfunctions in the natural space of the setting of the problem: cf the simple statements of Theorems 6.1 and 6.4

Formulation of the eigenvalue problem
The eigenvalue sequence: what is known and what is expected
State-of-the-art in the literature and new challenges
Structure of the paper
The first limit problem in the cell
The eigenvalue problem in the half-strip π
Properties of the principal eigenfunction
Asymptotics near collision points
Analysis of eigenfunctions in the original problem
Two scales asymptotic expansion and related issues
The second limit problem: a problem in Ω
The first term of the boundary layer
The second term of the boundary layer and the Steklov condition on Γ
Eigenpairs of the second limit problem: the Steklov problem
Transforming the asymptotic expansions of eigenfunctions
A two scale convergence result
Estimation of asymptotic remainders
Abstract formulation of the ε-dependent eigenvalue problem
Choosing near eigenvalues and eigenvectors
Estimating discrepancies
The intermediate result on asymptotics
The convergence theorem
Reformulation of the ε-dependent eigenvalue problem
Passing to the limit in the integral identity
Asymptotics of eigenvalues and eigenfunctions
Asymptotic splitting of eigenvalues
Asymptotic forms for eigenfunctions
The homogeneous Kondratiev norms
The multi-scaled weighted norms
Weighted spaces with detached asymptotics
Full Text
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