2020
DOI: 10.1137/19m1274651
|View full text |Cite
|
Sign up to set email alerts
|

Wave Enhancement Through Optimization of Boundary Conditions

Abstract: It is well-known that changing boundary conditions for the Laplacian from Dirichlet to Neumann can result in significant changes to the associated eigenmodes, while keeping the eigenvalues close. We present a new and efficient approach for optimizing the transmission signal between two points in a cavity at a given frequency, by changing boundary conditions. The proposed approach makes use of recent results on the monotonicity of the eigenvalues of the mixed boundary value problem and on the sensitivity of the… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1
1
1

Citation Types

0
12
0

Year Published

2020
2020
2023
2023

Publication Types

Select...
6
2

Relationship

3
5

Authors

Journals

citations
Cited by 8 publications
(12 citation statements)
references
References 16 publications
0
12
0
Order By: Relevance
“…For example in [2], Steklov boundary conditions are studied. Moreover, mixed boundaries as they are studied in [1] move the singularity in k of the scattered wave away from k = 0. Thus with mixed boundaries we might achieve a better control of the resonance effect.…”
Section: Discussionmentioning
confidence: 99%
“…For example in [2], Steklov boundary conditions are studied. Moreover, mixed boundaries as they are studied in [1] move the singularity in k of the scattered wave away from k = 0. Thus with mixed boundaries we might achieve a better control of the resonance effect.…”
Section: Discussionmentioning
confidence: 99%
“…The main purpose of this section is to prove the following theorem, which establishes that the quasi-eigenvalues introduced in Definitions 2. 3 We will prove Theorem 4.1 by constructing an appropriate sequence of quasimodes which we first define in a very general setting.…”
Section: General Approachmentioning
confidence: 99%
“…From [26,Theorem 4.10], and the fact that the first mixed Dirichlet -Neumann eigenvalue is not zero [6], as long as Γ S is not empty, we have that Z Γ S (x S , ·) ∈ H 1 (Ω) exists. From Lemma 3.1, we see that U λ Γ S (x S , ·) ∈ H 1 (Ω) exists.…”
Section: Asymptotics For the Steklov-neumann Functionmentioning
confidence: 99%