Section XI.4

The Essential Spectrum

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Problem XI.4.1

Show that the material of this section is only significant for infinite dimensional Hilbert spaces by showing that the essential spectrum of every operator on H\mathcal{H} is non-empty if and only if H\mathcal{H} is infinite dimensional.

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Problem XI.4.2

Let GG be a bounded region in C\mathbb {C} such that ∂G=∂[cl G]\partial G = \partial [\mathrm{cl}\ G] and let ϕ\phi be a function that is analytic in a neighborhood of cl G\mathrm{cl}\ G. Define A:La2(G)→La2(G)A: L_a^2(G) \to L_a^2(G) by Af=ϕfAf = \phi f. Find all of the parts of the spectrum of AA.

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Problem XI.4.3

(Fillmore, Stampfli, and Williams [1972].) If λ∈σle(A)\lambda \in \sigma_{le}(A), then there is a projection PP, having infinite rank, such that π(A−λ)π(P)=0\pi (A - \lambda )\pi (P) = 0.

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Problem XI.4.4

(Fillmore, Stampfli, and Williams [1972].) Let A∈B(H)A \in \mathcal{B}(\mathcal{H}).

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(a)

If AA has a cyclic vector ee, show that dim⁡{Ae,A2e,…}⊥≤1\dim \left\{ Ae, A^2e, \ldots \right\}^\perp \le 1.

(b)

Let λ∈σle(A∗)\lambda \in \sigma_{le}(A^*). If ε>0\varepsilon > 0, let f1,f2f_1, f_2 be orthonormal vectors such that ∥(A∗−λ)fj∥<ε\left\| (A^* - \lambda )f_j\right\| < \varepsilon for j=1,2j = 1, 2 and let P=P = the projection onto ⋁{f1,f2}\bigvee \left\{ f_1, f_2\right\}. Put B=λˉP+(1−P)AB = \bar{\lambda }P + (1 - P)A. Show that ∥B−A∥<2ε\left\| B - A\right\| < 2\varepsilon.

(c)

Show that the noncyclic operators are dense in B(H)\mathcal{B}(\mathcal{H}) if dim⁡H>1\dim \mathcal{H} > 1.

Problem XI.4.5

Let A∈FA \in \mathcal{F} and suppose ff is analytic in a neighborhood of σ(A)\sigma (A) and does not vanish on σe(A)\sigma_e(A). Show that f(A)∈Ff(A) \in \mathcal{F} and find ind⁡f(A)\operatorname {ind} f(A).

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Problem XI.4.6

Let SS be the unilateral shift and let ff be an analytic function in a neighborhood of cl D\mathrm{cl}\ \mathbb {D} such that f(z)≠0f(z) \ne 0 if ∣z∣=1\left|z\right| = 1. Let γ(t)=f(exp⁡(2πit))\gamma (t) = f(\exp (2\pi i t)), 0≤t≤10 \le t \le 1. Show that σe(f(S))=f(∂D)={γ(t):0≤t≤1}\sigma_e(f(S)) = f(\partial \mathbb {D}) = \left\{ \gamma (t): 0 \le t \le 1\right\} and that if λ∉f(∂D)\lambda \notin f(\partial \mathbb {D}), ind⁡(f(S)−λ)=−n(γ;λ)\operatorname {ind}(f(S) - \lambda ) = -n(\gamma ; \lambda ), where n(γ;λ)=n(\gamma ; \lambda ) = the winding number of γ\gamma about λ\lambda. Moreover, show that if ind⁡(f(S)−λ)=0\operatorname {ind}(f(S) - \lambda ) = 0, then λ∉σ(f(S))\lambda \notin \sigma (f(S)).

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Problem XI.4.7

Let SS be the operator defined in Example 2.11 where G=DG = \mathbb {D}. Show that there is a compact operator KK such that S+KS + K is unitarily equivalent to the unilateral shift.

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Problem XI.4.8

If SS is the unilateral shift, show that for every ε>0\varepsilon > 0 there is a rank one operator FF with ∥F∥<ε\left\| F\right\| < \varepsilon such that σ(S∗⊕S+F)=∂D\sigma (S^* \oplus S + F) = \partial \mathbb {D}.

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Problem XI.4.9

Let GG be an open connected subset of σ(A)∖σle(A)∪σre(A)\sigma (A) \setminus \sigma_{le}(A) \cup \sigma_{re}(A) and suppose λ0∈G\lambda_0 \in G such that ind⁡(A−λ0)=0\operatorname {ind}(A - \lambda_0) = 0. Show that there is a finite rank operator FF such that A+F−λ0A + F - \lambda_0 is invertible. Show that A+F−λA + F - \lambda is invertible for every λ\lambda in GG.

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