2010
DOI: 10.1016/j.jcp.2010.07.040
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Optimization of spectral functions of Dirichlet–Laplacian eigenvalues

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Cited by 25 publications
(14 citation statements)
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“…Our BFGS implementation in hanso has been used to solve a variety of practical nonsmooth problems, such as a condition geodesic problem [3] and shape optimization for spectral functions of Dirichlet-Laplacian operators [40].…”
Section: Softwarementioning
confidence: 99%
“…Our BFGS implementation in hanso has been used to solve a variety of practical nonsmooth problems, such as a condition geodesic problem [3] and shape optimization for spectral functions of Dirichlet-Laplacian operators [40].…”
Section: Softwarementioning
confidence: 99%
“…Doing this truncation, we don't perturb the eigenvalues too much. B. Osting gives an estimate of this error in [23]. In this way we can represent a good approximation of the boundary of a star convex shape by a finite number of parameters.…”
Section: Introductionmentioning
confidence: 99%
“…There are several available methods for solving eigenvalues problems on general domains, including the finite difference [33], finite element [29,7], boundary integral [12], method of particular solutions [22,6,13,40], and meshless methods [3]. In this paper we use the finite element method [33,12,29,7].…”
Section: Methodsmentioning
confidence: 99%
“…Results min |Ω|=1 λ k k = 1: Minimizer is a ball (Rayleigh-Faber-Krahn); see [25,4] k = 2: Minimizer is union of 2 balls of equal volume (Krahn-Szegö); see [25,4] k = 3: Minimizer is connected and a ball is a local minimizer [49] k = 4: Candidate minimizer is union of two balls with different volumes; see [25] k ≥ 5: Numerical results: k = 3 : 10 [43] and k = 5 : 15 [3] min |Ω|=1 (1 − γ)λ k + γλ k+1 For k = 1, only γ = 1 is disconnected [49] k = 1 and γ ∈ [0, 1]: numerical results [49] k = 1 : 14 and γ = 1 2 : numerical results [2] k = 1 : 5 and γ ∈ [0, 1], present work max Ω λ k λ 1 k = 2: Maximizer is a ball (Ashbaugh-Benguria); see [5] Numerical results: k = 3, [35]; k = 3 : 13, [40]; k = 3 : 14, [2] where Λ(Ω) = {λ k (Ω)} ∞ k=1 are the Laplace-Dirichlet eigenvalues of Ω. (See section 2 for a mathematical formulation.)…”
Section: Problemmentioning
confidence: 99%
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