224 research outputs found

    A trace formula for functions of contractions and analytic operator Lipschitz functions

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    In this note we study the problem of evaluating the trace of f(T)f(R)f(T)-f(R), where TT and RR are contractions on Hilbert space with trace class difference, i.e., TRS1T-R\in\boldsymbol{S}_1 and ff is a function analytic in the unit disk D{\Bbb D}. It is well known that if ff is an operator Lipschitz function analytic in D{\Bbb D}, then f(T)f(R)S1f(T)-f(R)\in\boldsymbol{S}_1. The main result of the note says that there exists a function ξ\boldsymbol{\xi} (a spectral shift function) on the unit circle T{\Bbb T} of class L1(T)L^1({\Bbb T}) such that the following trace formula holds: trace(f(T)f(R))=Tf(ζ)ξ(ζ)dζ\operatorname{trace}(f(T)-f(R))=\int_{\Bbb T} f'(\zeta)\boldsymbol{\xi}(\zeta)\,d\zeta, whenever TT and RR are contractions with TRS1T-R\in\boldsymbol{S}_1 and ff is an operator Lipschitz function analytic in D{\Bbb D}.Comment: 6 page

    On the unitary equivalence of absolutely continuous parts of self-adjoint extensions

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    The classical Weyl-von Neumann theorem states that for any self-adjoint operator AA in a separable Hilbert space H\mathfrak H there exists a (non-unique) Hilbert-Schmidt operator C=CC = C^* such that the perturbed operator A+CA+C has purely point spectrum. We are interesting whether this result remains valid for non-additive perturbations by considering self-adjoint extensions of a given densely defined symmetric operator AA in H\mathfrak H and fixing an extension A0=A0A_0 = A_0^*. We show that for a wide class of symmetric operators the absolutely continuous parts of extensions A~=A~\widetilde A = {\widetilde A}^* and A0A_0 are unitarily equivalent provided that their resolvent difference is a compact operator. Namely, we show that this is true whenever the Weyl function M()M(\cdot) of a pair {A,A0}\{A,A_0\} admits bounded limits M(t) := \wlim_{y\to+0}M(t+iy) for a.e. tRt \in \mathbb{R}. This result is applied to direct sums of symmetric operators and Sturm-Liouville operators with operator potentials
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