Abstract:Let S be the orthogonal sum of infinitely many pairwise unitarily equivalent symmetric operators with non-zero deficiency indices. Let J be an open subset of R. If there exists a self-adjoint extension S 0 of S such that J is contained in the resolvent set of S 0 and the associated Weyl function of the pair {S, S 0 } is monotone with respect to J, then for any selfadjoint operator R there exists a self-adjoint extension S such that the spectral parts S J and R J are unitarily equivalent. It is shown that for a… Show more
“…The assumption that A admits a scalar-type Weyl function has far going spectral implications beyond the gap. In [3] it was conjectured that already the monotonicity assumption is sufficient to solve the Problem 1.2. In the following we make a first step to verify this conjecture for the special case that the deficiency indices are finite.…”
Section: N(a) the Decomposition (10) Is Not Uniquementioning
Abstract. Let A be a closed symmetric operator on a separable Hilbert space with equal finite deficiency indices n(A) < ∞ and let J be an open subset of R. It is shown that if there is a self-adjoint extension A0 of A such that J is contained in the resolvent set of A0 and the associated Weyl function of the pair {A, A0} is monotone with respect to J, then for any self-adjoint operator R on some separable Hilbert space R obeying dim(ER(J)R) ≤ n(A) there exists a self-adjoint extension A such that the spectral parts AJ and RJ are unitarily equivalent. The result generalizes a corresponding result of M.G. Krein for a single gap.
Mathematics Subject Classification (2000). Primary 47A56; Secondary 47B25.
“…The assumption that A admits a scalar-type Weyl function has far going spectral implications beyond the gap. In [3] it was conjectured that already the monotonicity assumption is sufficient to solve the Problem 1.2. In the following we make a first step to verify this conjecture for the special case that the deficiency indices are finite.…”
Section: N(a) the Decomposition (10) Is Not Uniquementioning
Abstract. Let A be a closed symmetric operator on a separable Hilbert space with equal finite deficiency indices n(A) < ∞ and let J be an open subset of R. It is shown that if there is a self-adjoint extension A0 of A such that J is contained in the resolvent set of A0 and the associated Weyl function of the pair {A, A0} is monotone with respect to J, then for any self-adjoint operator R on some separable Hilbert space R obeying dim(ER(J)R) ≤ n(A) there exists a self-adjoint extension A such that the spectral parts AJ and RJ are unitarily equivalent. The result generalizes a corresponding result of M.G. Krein for a single gap.
Mathematics Subject Classification (2000). Primary 47A56; Secondary 47B25.
We consider a model of point-like interaction between electrons and bosons in a cavity. The electrons are relativistic and are described by a Dirac operator on a bounded interval while the bosons are treated by second quantization. The model fits into the extension theory of symmetric operators. Our main technical tool to handle the model is the so-called boundary triplet approach to extensions of symmetric operators. The approach allows explicit computation of the Weyl function.
“…), we refer, for instance, to [2], [3], [4], [11], [12], [13]- [19], [24]- [28], [33]- [39], [42], [44,Ch. 3], [45], [46,Ch.…”
Section: Ac([0 R]) Denotes the Set Of Absolutely Continuous Functionmentioning
confidence: 99%
“…That H θ 0 ,θ R is indeed a closed operator follows, for instance, from [29,Sect. XII.4], especially, by combining Lemma 5 (c) and the first part of the proof of Lemma 26 and noting that g(0), g (0) (resp., g(R), g (R)) are a complete set of boundary values for the minimal operator H min associated with the differential expression −d 2 …”
Abstract. We provide a systematic study of boundary data maps, that is, 2 × 2 matrix-valued Dirichlet-to-Neumann and more generally, Robin-to-Robin maps, associated with one-dimensional Schrödinger operators on a compact interval [0, R] with separated boundary conditions at 0 and R. Most of our results are formulated in the non-self-adjoint context.Our principal results include explicit representations of these boundary data maps in terms of the resolvent of the underlying Schrödinger operator and the associated boundary trace maps, Krein-type resolvent formulas relating Schrödinger operators corresponding to different (separated) boundary conditions, and a derivation of the Herglotz property of boundary data maps (up to right multiplication by an appropriate diagonal matrix) in the special self-adjoint case.
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