An alternative proof of the a priori tan⁡Θ\tanΘ Theorem

preprint2015arXivOpen access

Abstract

Let AA be a self-adjoint operator in a separable Hilbert space. Suppose that the spectrum of AA is formed of two isolated components σ0σ_0 and σ1σ_1 such that the set σ0σ_0 lies in a finite gap of the set σ1σ_1. Assume that VV is a bounded additive self-adjoint perturbation of AA, off-diagonal with respect to the partition spec(A)=σ0∪σ1{\rm spec}(A)=σ_0 \cup σ_1. It is known that if ∥V∥<2dist(σ0,σ1)\|V\|<\sqrt{2}{\rm dist}(σ_0,σ_1), then the spectrum of the perturbed operator L=A+VL=A+V consists of two disjoint parts ω0ω_0 and ω1ω_1 which originate from the corresponding initial spectral subsets σ0σ_0 and σ1σ_1. Moreover, for the difference of the spectral projections EA(σ0)E_A(σ_0) and EL(ω0)E_{L}(ω_0) of AA and LL associated with the spectral sets σ0σ_0 and ω0ω_0, respectively, the following sharp norm bound holds: ∥EA(σ0)−EL(ω0)∥≤sin⁡(arctan⁡∥V∥dist(σ0,σ1)).\|E_A(σ_0)-E_{L}(ω_0)\|\leq\sin\left(\arctan\frac{\|V\|}{{\rm dist}(σ_0,σ_1)}\right). In the present note, we give a new proof of this bound for ∥V∥<dist(σ0,σ1)\|V\|<{\rm dist}(σ_0,σ_1).

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