Operator models associated with singular perturbations (Q2777859)
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scientific article; zbMATH DE number 1718908
| Language | Label | Description | Also known as |
|---|---|---|---|
| English | Operator models associated with singular perturbations |
scientific article; zbMATH DE number 1718908 |
Statements
13 March 2002
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Weyl function
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generalized Nevanlinna function
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singular perturbation
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boundary triplet
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matrix polynomial
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operator model
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symmetric relation
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Pontryagin space
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coupling methods
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Schur complements
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Operator models associated with singular perturbations (English)
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Let \(S_0\) be a closed symmetric operator on a Hilbert space \(\mathfrak H_0\) with equal finite deficiency numbers \((d,d)\), and let \(M_0\) be the Weyl function of \(S_0\). For a monic \(d\times d\) matrix polynomial \(q\) and a selfadjoint \(d\times d\) matrix polynomial \(r\), the function \(M=r+q^\sharp M_0q\), where \(q^\sharp (\lambda)=q(\bar \lambda)^*\), is a generalized Nevanlinna function whose Nevanlinna kernel has \(dn\) negative squares. The authors construct an operator model to represent \(M\) as a Weyl function of a symmetric relation in a Pontryagin space \(\mathfrak H\) which contains \(\mathfrak H_0\) as a closed subspace. The construction is based on coupling methods involving models for sums and Schur complements of generalized Nevanlinna functions. The above model is used to obtain a (multivalued) operator interpretation of a singular finite rank perturbation of a selfadjoint operator.
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