Abstract
Singular finite rank perturbations of an unbounded self-adjoint operator A0 in a Hilbert space h0 are defined formally as A(α) = A0 + GαG*, where G is an injective linear mapping from H = Cd to the scale space h−k(A0), k ∈ N, of generalized elements associated with the selfadjoint operator A0, and where α is a self-adjoint operator in H. The cases k = 1 and k = 2 have been studied extensively in the literature with applications to problems involving point interactions or zero range potentials. The scalar case with k = 2n > 1 has been considered recently by various authors from a mathematical point of view. In this paper, singular finite rank perturbations A(α) in the general setting ran G ⊂ h−k(A0), k ∈ N, are studied by means of a recent operator model induced by a class of matrix polynomials. As an application, singular perturbations of the Dirac operator are considered.
Original language | English |
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Pages (from-to) | 349-384 |
Number of pages | 36 |
Journal | Mathematical physics analysis and geometry |
Volume | 6 |
Issue number | 4 |
DOIs | |
Publication status | Published - Apr-2003 |
Keywords
- singular finite rank perturbations
- extension theory
- Krein's formula
- boundary triplet
- Weyl function
- generalized Nevanlinna function
- operator model
- RANK-ONE PERTURBATIONS
- NEVANLINNA FUNCTIONS
- PONTRYAGIN SPACE
- EXTENSIONS
- MODELS