The spectral density of a difference of spectral projections

preprint2015arXivOpen access

Abstract

Let H0H_0 and HH be a pair of self-adjoint operators satisfying some standard assumptions of scattering theory. It is known from previous work that if λλ belongs to the absolutely continuous spectrum of H0H_0 and HH, then the difference of spectral projections D(λ)=1(−∞,0)(H−λ)−1(−∞,0)(H0−λ)D(λ)=1_{(-\infty,0)}(H-λ)-1_{(-\infty,0)}(H_0-λ) in general is not compact and has non-trivial absolutely continuous spectrum. In this paper we consider the compact approximations Dε(λ)D_\varepsilon(λ) of D(λ)D(λ), given by Dε(λ)=ψε(H−λ)−ψε(H0−λ),D_\varepsilon(λ)=ψ_\varepsilon(H-λ)-ψ_\varepsilon(H_0-λ), where ψε(x)=ψ(x/ε)ψ_\varepsilon(x)=ψ(x/\varepsilon) and ψ(x)ψ(x) is a smooth real-valued function which tends to ∓1/2\mp1/2 as x→±∞x\to\pm\infty. We prove that the eigenvalues of Dε(λ)D_\varepsilon(λ) concentrate to the absolutely continuous spectrum of D(λ)D(λ) as ε→+0\varepsilon\to+0. We show that the rate of concentration is proportional to ∣log⁡ε∣|\log\varepsilon| and give an explicit formula for the asymptotic density of these eigenvalues. It turns out that this density is independent of ψψ. The proof relies on the analysis of Hankel operators.

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