The Spectrum of Delay Differential Equations with Multiple Hierarchical Large Delays

We prove that the spectrum of the linear delay differential equation \(x'(t)=A_{0}x(t)+A_{1}x(t-\tau_{1})+\ldots+A_{n}x(t-\tau_{n})\) with multiple hierarchical large delays \(1\ll\tau_{1}\ll\tau_{2}\ll\ldots\ll\tau_{n}\) splits into two distinct parts: the strong spectrum and the pseudo-contin...

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Bibliographic Details
Published inarXiv.org
Main Authors Ruschel, Stefan, Yanchuk, Serhiy
Format Paper
LanguageEnglish
Published Ithaca Cornell University Library, arXiv.org 17.12.2019
Subjects
Asymptotic properties
Convergence
Delay
Destabilization
Differential equations
Eigenvalues
Evaporation
Rescaling
Spectra
Structural hierarchy
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Summary:We prove that the spectrum of the linear delay differential equation \(x'(t)=A_{0}x(t)+A_{1}x(t-\tau_{1})+\ldots+A_{n}x(t-\tau_{n})\) with multiple hierarchical large delays \(1\ll\tau_{1}\ll\tau_{2}\ll\ldots\ll\tau_{n}\) splits into two distinct parts: the strong spectrum and the pseudo-continuous spectrum. As the delays tend to infinity, the strong spectrum converges to specific eigenvalues of \(A_{0}\), the so-called asymptotic strong spectrum. Eigenvalues in the pseudo-continuous spectrum however, converge to the imaginary axis. We show that after rescaling, the pseudo-continuous spectrum exhibits a hierarchical structure corresponding to the time-scales \(\tau_{1},\tau_{2},\ldots,\tau_{n}.\) Each level of this hierarchy is approximated by spectral manifolds that can be easily computed. The set of spectral manifolds comprises the so-called asymptotic continuous spectrum. It is shown that the position of the asymptotic strong spectrum and asymptotic continuous spectrum with respect to the imaginary axis completely determines stability. In particular, a generic destabilization is mediated by the crossing of an \(n\)-dimensional spectral manifold corresponding to the timescale \(\tau_{n}\).
ISSN:2331-8422