2012
DOI: 10.1002/mana.201100172
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Oscillation and spectral theory for linear Hamiltonian systems with nonlinear dependence on the spectral parameter

Abstract: Key words Linear Hamiltonian system, self-adjoint eigenvalue problem, proper focal point, conjoined basis, finite eigenvalue, oscillation, controllability, normality, quadratic functional MSC (2010) 34L05, 34C10, 49N10, 93B60, 34L10In this paper, we consider linear Hamiltonian differential systems which depend in general nonlinearly on the spectral parameter and with Dirichlet boundary conditions. Our results generalize the known theory of linear Hamiltonian systems in two respects. Namely, we allow nonlinear … Show more

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Cited by 20 publications
(30 citation statements)
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References 15 publications
(23 reference statements)
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“…More precisely, we provide examples illustrating the Downloaded 11/17/14 to 130.113.76. 6. Redistribution subject to SIAM license or copyright; see http://www.siam.org/journals/ojsa.php fact that the conclusions of Theorem 2.1 do not hold when the rank of R 2 (t) changes.…”
mentioning
confidence: 75%
See 1 more Smart Citation
“…More precisely, we provide examples illustrating the Downloaded 11/17/14 to 130.113.76. 6. Redistribution subject to SIAM license or copyright; see http://www.siam.org/journals/ojsa.php fact that the conclusions of Theorem 2.1 do not hold when the rank of R 2 (t) changes.…”
mentioning
confidence: 75%
“…It is well known that discrete symplectic systems constitute a natural analogue of continuous time (differential) linear Hamiltonian systems; see [6,8,20,23]. Symplectic systems with the nonlinear dependence on λ, as in (S λ ), were recently introduced by the second author in [24] in connection with the eigenvalue problem with Dirichlet boundary conditions…”
mentioning
confidence: 99%
“…However, in [5] a certain strict normality assumption is needed to prove that the eigenvalues are isolated and bounded from below, which is not required in the present paper. Our results can also be regarded as a discrete time analogue of the corresponding theory in [9] for the continuous time linear Hamiltonian systems…”
Section: Introductionmentioning
confidence: 86%
“…These equations are considered e.g. in , , , . Remark The assumptions of Theorem 4.1 imply that the finite eigenvalues of (E) and (E̲) are isolated and bounded from below, compare with [, Corollary 3.3 and Theorem 3.5]. Thus, if we denote by <λ1λ2λkand<λ̲1λ̲2λ̲kthe finite eigenvalues of (E) and (E̲), respectively, then inequality is equivalent with λ̲kλkforallkN,whenever the k ‐th finite eigenvalues of (E) and (E̲) exist.…”
Section: Comparison Of Finite Eigenvaluesmentioning
confidence: 95%
“…Let nN be fixed. Let be given n×n piecewise continuously differentiable ()Cp1 functions A(·,·), B(·,·), C(·,·) on [a,b]×R such that B(t,λ) and C(t,λ) are symmetric, B(t,λ)0forallt[a,b],λR,and the Hamiltonian matrix H(·,·) defined in satisfies the following, see [, Assumption (2.1)]. There exist a partition a=τ0<<τm=b of [a,b] and a partition <<λk<λk+1<< of double-struckR with no finite accumulation point such that scriptH is continuous on [τi,τi+1]×R for every i=0,,m1, trueḢ is continuous on …”
Section: Oscillation and Spectral Properties Of Linear Hamiltonian Symentioning
confidence: 99%