Operator Theory, Analysis and Mathematical Physics
DOI: 10.1007/978-3-7643-8135-6_9
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Functional Model of a Class of Non-selfadjoint Extensions of Symmetric Operators

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Cited by 25 publications
(65 citation statements)
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“…It has been shown, indeed, that a key point in the development of the scattering theory for the possibly non-selfadjoint pair {H 0 , H 1 } is the existence of the strong limit on the real axis of the characteristic functions associated with H i=0,1 (e.g. in [29] and [30]). In particular, the Theorem 4.1 in [29] makes use of this assumption to study the existence of the related wave operators.…”
Section: Generalized Eigenfunctions Expansionmentioning
confidence: 99%
“…It has been shown, indeed, that a key point in the development of the scattering theory for the possibly non-selfadjoint pair {H 0 , H 1 } is the existence of the strong limit on the real axis of the characteristic functions associated with H i=0,1 (e.g. in [29] and [30]). In particular, the Theorem 4.1 in [29] makes use of this assumption to study the existence of the related wave operators.…”
Section: Generalized Eigenfunctions Expansionmentioning
confidence: 99%
“…It is convenient to use representation for A in the form (2.3) for z ∈ C − and in the form (2.4) for z ∈ C + . The interested reader is referred to [44] Theorem 2.2, where analogous calculations were carried out for a special case of operator A.…”
Section: Boundary Operators Letmentioning
confidence: 99%
“…It was already successfully applied (without a proof) to the study of nondissipative operators from a fairly wide class in [42,43], where the notion of local absolutely continuous and singular subspaces was examined and utilized for the subsequent study of scattering theory for a pair of nonselfadjoint operators. Owing to the generic form of operator under consideration, results obtained in the current paper cover both cases of the model for nonselfadjoint additive perturbations [28] and for extensions of symmetric operators [44]. As a direct consequence, considerations below can be used for study of selfadjoint operators subject to a nonselfadjoint additive perturbations in combination with nonselfadjoint boundary conditions.…”
Section: Introductionmentioning
confidence: 99%
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