2015
DOI: 10.1137/140964631
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Differential Equations for Real-Structured Defectivity Measures

Abstract: Let A be a real matrix with all distinct eigenvalues. We propose a new method for the computation of the distance w_R(A) of the matrix A from the set of real defective matrices, i.e., the set of those real matrices with at least one multiple eigenvalue with algebraic multiplicity larger than its geometric multiplicity. For 0 < ε ≤ w_R(A), this problem is closely related to the computation of the most ill-conditioned ε-pseudoeigenvalues of A, that is, points in the ε-pseudospectrum of A characterized by the hig… Show more

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Cited by 5 publications
(4 citation statements)
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“…When scriptS=Cn×n, i.e., when A has no particular structure, the perturbations that affect the eigenvalue λ of A the most, relative to the norm of the perturbation, are multiples of the rank‐one matrices . The Wilkinson disks for the different eigenvalues are disjoint if the radius t of the disks is smaller than the distance ϵ ∗ from defectivity of the matrix A , ϵ=inf{ABF:Bdouble-struckCn×nis defective}. Analogously, in case scriptSCn×n the threshold is the structured distance from defectivity ϵscriptS of A , ϵS=inf{ABF:BSis defective}. Clearly, ϵscriptSϵ;see, e.g., for details. In the structured case, the rank‐one Wilkinson perturbations are projected as described in Section 3.…”
Section: Approximated Structured ϵ‐Pseudospectramentioning
confidence: 98%
“…When scriptS=Cn×n, i.e., when A has no particular structure, the perturbations that affect the eigenvalue λ of A the most, relative to the norm of the perturbation, are multiples of the rank‐one matrices . The Wilkinson disks for the different eigenvalues are disjoint if the radius t of the disks is smaller than the distance ϵ ∗ from defectivity of the matrix A , ϵ=inf{ABF:Bdouble-struckCn×nis defective}. Analogously, in case scriptSCn×n the threshold is the structured distance from defectivity ϵscriptS of A , ϵS=inf{ABF:BSis defective}. Clearly, ϵscriptSϵ;see, e.g., for details. In the structured case, the rank‐one Wilkinson perturbations are projected as described in Section 3.…”
Section: Approximated Structured ϵ‐Pseudospectramentioning
confidence: 98%
“…, [1,2,9,10] for details. In the structured case, the rank-one Wilkinson perturbations (2.1) are projected as described in Section 3.…”
Section: Approximated Structured ε-Pseudospectramentioning
confidence: 99%
“…This completes the proof. Similarly to [BGMN13] we state the following uniqueness result for sufficiently small ε.…”
mentioning
confidence: 93%