Section XI.1

The Spectrum Revisited

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Problem XI.1.1

Let SS be the unilateral shift of multiplicity 11 on l2(N)l^2(\mathbb {N}) and find σl(S)\sigma_l(S) and σr(S)\sigma_r(S).

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Problem XI.1.2

The compression spectrum of AA, σc(A)\sigma_c(A), is defined by σc(A)={λ∈C:ran(A−λ) is not dense in H}\sigma_c(A) = \left\{ \lambda \in \mathbb {C}: \mathrm{ran}(A - \lambda ) \text{ is not dense in } \mathcal{H}\right\}. Show:

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(a)

λ∈σc(A)\lambda \in \sigma_c(A) if and only if λˉ∈σp(A∗)\bar{\lambda } \in \sigma_p(A^*).

(b)

σc(A)⊆σr(A)\sigma_c(A) \subseteq \sigma_r(A), but this inclusion may be proper.

(c)

σc(A)\sigma_c(A) is not necessarily closed.

(d)

σ(A)=σap(A)∪σc(A)\sigma (A) = \sigma_{ap}(A) \cup \sigma_c(A).

Problem XI.1.3

If A∈B(H)A \in \mathcal{B}(\mathcal{H}) and f∈Hol(A)f \in \mathrm{Hol}(A), then f(σp(A))⊆σp(f(A))f(\sigma_p(A)) \subseteq \sigma_p(f(A)). If ff is not constant on any component of its domain, then f(σp(A))=σp(f(A))f(\sigma_p(A)) = \sigma_p(f(A)).

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Problem XI.1.4

If A∈B(H)A \in \mathcal{B}(\mathcal{H}) and f∈Hol(A)f \in \mathrm{Hol}(A), then f(σap(A))=σap(f(A))f(\sigma_{ap}(A)) = \sigma_{ap}(f(A)).

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