2001
DOI: 10.1016/s0377-0427(00)00663-4
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Limit points of eigenvalues of truncated tridiagonal operators

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Cited by 12 publications
(10 citation statements)
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“…. , a n−1 , u n ) for a sequence u in T. A recommendable choice is the sequence u = u w given in (19) that fixes a common eigenvalue w for all the finite matrices, because it permits us to control the only possible strong limit point that, according to Theorem 4.17, can lie outside supp . In this case Theorem 4.18 proves that the double limit points coincide with supp ∪ {w}, so the computation of the eigenvalues for pairs of consecutive matrices can be used to eliminate those weak limit points that are spurious points of supp .…”
Section: Proposition 415mentioning
confidence: 99%
“…. , a n−1 , u n ) for a sequence u in T. A recommendable choice is the sequence u = u w given in (19) that fixes a common eigenvalue w for all the finite matrices, because it permits us to control the only possible strong limit point that, according to Theorem 4.17, can lie outside supp . In this case Theorem 4.18 proves that the double limit points coincide with supp ∪ {w}, so the computation of the eigenvalues for pairs of consecutive matrices can be used to eliminate those weak limit points that are spurious points of supp .…”
Section: Proposition 415mentioning
confidence: 99%
“…Information about Λ(T ) is of great importance not only from the point of view of operator theory, but also for the theory of continued fractions, orthogonal polynomials and numerical analysis (see [13] and the references therein).…”
Section: Introductionmentioning
confidence: 99%
“…In the bounded case several sufficient conditions for Λ(T ) = σ(T ) can be found in the literature, but not much is known in the unbounded case (see [12,13], also [4,5] for related problems concerning non-symmetric tridiagonal operators, and [6] for extensions to unitary CMV operators). In particular, the authors of [12] established sufficient conditions for Λ(T ) = σ(T ) when b n is divergent, which regard the limits of some functions of a n , b n .…”
Section: Introductionmentioning
confidence: 99%
“…Second, at any time t ≥ 0, L(t) is a compact perturbation of the discrete free Schrrödinger operator L 0 that has a n ≡ 1 2 , b n ≡ 0, and σ L 0 = σ ac L 0 = [−1, 1]. As proven in [26], these two facts imply: Proposition 3.4 (Theorem 2.3, [26]). Let Z(L) denote the set of all limit points of ∞ N =1 σ L N .…”
Section: The Numerical Schemementioning
confidence: 83%