2015
DOI: 10.1016/j.laa.2014.11.030
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On essential spectra of singular linear Hamiltonian systems

Abstract: The paper is concerned with essential spectra of singular linear Hamiltonian systems of arbitrary order with arbitrary equal defect indices. Several sufficient conditions for the essential spectral points are given in terms of the number of linearly independent square integrable solutions of the corresponding Hamiltonian system, and a sufficient and necessary condition for the essential spectral points is obtained for Hamiltonian systems of even-order with one singular endpoint. An advantage of these results i… Show more

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Cited by 16 publications
(12 citation statements)
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References 25 publications
(64 reference statements)
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“…For every a >0, consider the restriction τ a of τ to [ a , ∞ ). We have σ e ( τ )= σ e ( τ a ) by Sun and Shi, Theorem 4.1 since equation τ y = λ y is a special case of the Hamiltonian systems discussed in Sun and Shi and the numbers of linearly independent square integrable solutions of τ y = λ y and τ a y = λ y are equal. Let T a ,0 be the preminimal operator corresponding to τ a defined similarly as T 0 .…”
Section: Resultsmentioning
confidence: 94%
See 2 more Smart Citations
“…For every a >0, consider the restriction τ a of τ to [ a , ∞ ). We have σ e ( τ )= σ e ( τ a ) by Sun and Shi, Theorem 4.1 since equation τ y = λ y is a special case of the Hamiltonian systems discussed in Sun and Shi and the numbers of linearly independent square integrable solutions of τ y = λ y and τ a y = λ y are equal. Let T a ,0 be the preminimal operator corresponding to τ a defined similarly as T 0 .…”
Section: Resultsmentioning
confidence: 94%
“…Then yfalse(tfalse)=false(γfalse(sfalse)truey˜false(sfalse)false)γfalse(sfalse), and hence trueτ˜αy is transformed into τ1,γ(y˜)(s)=γ(s)(γ(s)y˜(s))+γ1(s)v(s)y˜(s),s[0,), From limsγfalse(sfalse)=1, we get that y ∈ L 2 [0, ∞ ) if and only if truey˜Lγ12false[0,false), and hence the number of linearly independent solutions of equation trueτ˜αy=λy in L 2 [0, ∞ ) is equal to that of linearly independent solutions of equation τ1,γtruey˜=λtruey˜ in Lγ12false[0,false). Then, σefalse(trueτ˜αfalse)=σefalse(τ1,γfalse) by Sun and Shi, Theorem 4.1. Using lims...…”
Section: Resultsmentioning
confidence: 99%
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“…The study of fundamental theory of regular difference equations has a long history and their spectral theory has formed a relatively complete theoretical system such as eigenvalue problems, orthogonality of eigenfunctions and expansion theory (cf., [2,17,27,36,39,41]). Spectral problems for singular difference equations were firstly studied by Atkinson [2] in 1964, and some significant progresses have been made since then (cf., e.g., [5,6,8,16,21,22,24,25,28,32,33,37,38]). Especially, research on spectral theory of singular discrete Hamiltonian systems has attracted a great deal of interest and some good results have been obtained (cf., [22,24,25,28,37,38], and references cited therein).…”
Section: Introductionmentioning
confidence: 99%
“…Spectra of singular symmetric differential operators have been studied intensively by researchers using various methods such as the asymptotic analysis, the oscillation theory, and the singular sequence approaches, see , , , , , . Especially, spectra of singular symmetric differential operators can be considered using the numbers of linearly independent square‐integrable solutions (cf., e.g., , , , , , , , ). An advantage of this method is the availability of numerous tools in the fundamental theory of differential equations for the study of spectra of differential operators.…”
Section: Introductionmentioning
confidence: 99%