Tridiagonal matrix representations of cyclic self-adjoint operators. II

Scattering Matrix and Functions of Self-adjoint Operators

In the scattering theory framework, we consider a pair of operators H0, H. For a continuous function φ vanishing at infinity, we set φδ(·) = φ(·/δ) and study the spectrum of the difference φδ(H − λ)− φδ(H0 − λ) for δ → 0. We prove that if λ is in the absolutely continuous spectrum of H0 and H, then the spectrum of this difference converges to a set that can be explicitly described in terms of (...

Diagonals of Self-adjoint Operators

The eigenvalues of a self-adjoint n×n matrix A can be put into a decreasing sequence λ = (λ1, . . . , λn), with repetitions according to multiplicity, and the diagonal of A is a point of R that bears some relation to λ. The Schur-Horn theorem characterizes that relation in terms of a system of linear inequalities. We prove an extension of the latter result for positive trace-class operators on ...

Non-self-adjoint Differential Operators

We describe methods which have been used to analyze the spectrum of non-self-adjoint differential operators, emphasizing the differences from the self-adjoint theory. We find that even in cases in which the eigenfunctions can be determined explicitly, they often do not form a basis; this is closely related to a high degree of instability of the eigenvalues under small perturbations of the opera...

Adjoints and Self-Adjoint Operators

Let V and W be real or complex finite dimensional vector spaces with inner products 〈·, ·〉V and 〈·, ·〉W , respectively. Let L : V → W be linear. If there is a transformation L∗ : W → V for which 〈Lv,w〉W = 〈v, Lw〉V (1) holds for every pair of vectors v ∈ V and w in W , then L∗ is said to be the adjoint of L. Some of the properties of L∗ are listed below. Proposition 1.1. Let L : V →W be linear. ...

On Families of Self Adjoint Operators