Abstract
Let A 0 be an unbounded self-adjoint operator in a Hilbert space H 0 and let χ be a generalized element of order — m — 1 in the rigging associated with A 0 and the inner product 〈·, ·〉0 of H 0. In [S1, S2, S3] operators H t, t · R ∪ ∞, are defined which serve as an interpretation for the family of operators A 0 + t -1 〈·, χ〉0 χ. The second summand here contains the inner singularity mentioned in the title. The operators H t act in Pontryagin spaces of the form π m = H 0⊕C m⊕C mwhere the direct summand space Cm ⊕ Cmis provided with an indefinite inner product. They can be interpreted both as a canonical extension of some symmetric operator S in π m and also as extensions of a one-dimensional restriction S 0 of A 0 in H 0 and hence they can be characterized by a class of Straus extensions of S 0 as well as via M.G. Krein’s formulas for (generalized) resolvents. In this paper we describe both these realizations explicitly and study their spectral properties. A main role is played by a special class of Q-functions. Factorizations of these functions correspond to the separation of the nonpositive type spectrum from the positive spectrum of H t. As a consequence, in Subsection 7.3 a family of self-adjoint Hilbert space operators is obtained which can serve as a nontrivial quantum model associated with the operators A 0 + t -1 〈·, χ〉0 χ.
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The research of Heinz Langer was supported by the Fonds zur Förderung der wissenschaftlichen Forschung of Austria, Project P 12176 MAT.
The research of Yuri Shondin was supported by the Netherlands Organization for Scientific Research NWO (NB 61-377) and by INTAS (93-0249-EXT).
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Dijksma, A., Langer, H., Shondin, Y., Zeinstra, C. (2000). Self-adjoint Operators with Inner Singularities and Pontryagin Spaces. In: Adamyan, V.M., et al. Operator Theory and Related Topics. Operator Theory: Advances and Applications, vol 118. Birkhäuser, Basel. https://doi.org/10.1007/978-3-0348-8413-6_8
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