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Upper Triangular Operator Matrices, SVEP and Browder, Weyl Theorems
Authors:B P Duggal
Institution:(1) 8 Redwood Grove Ealing, London, W5 4SZ, United Kingdom
Abstract:A Banach space operator TB(χ) is polaroid if points λ ∈ iso σ(T) are poles of the resolvent of T. Let $$\sigma_a(T), \sigma_w(T), \sigma_{aw}(T), \sigma_{SF_+}(T)\, \rm{and}\,\sigma_{SF_-}(T)$$ denote, respectively, the approximate point, the Weyl, the Weyl essential approximate, the upper semi–Fredholm and lower semi–Fredholm spectrum of T. For A, B and CB(χ), let M C denote the operator matrix $$\left( {\begin{array}{ll}  A & C \\  0 & B \\ \end{array} } \right)$$. If A is polaroid on $$\pi_{0}(M_{C}) = \{{\lambda \in {\rm iso}\, \sigma(M_{C}) : 0 < {\rm dim} (M_{C} - \lambda)^{-1}(0) < \infty}\}$$, M 0 satisfies Weyl’s theorem, and A and B satisfy either of the hypotheses (i) A has SVEP at points $$\lambda \in \sigma_{w}(M_{0}) \backslash {\sigma_{SF_{+}}}+(A)$$ and B has SVEP at points $$\mu \in \sigma_{w}(M_{0}) \backslash {\sigma_{SF_{-}}}(B)$$, or, (ii) both A and A* have SVEP at points $$\lambda \in \sigma_{w}(M_{0}) \backslash {\sigma_{SF_{+}}}(A)$$, or, (iii) A* has SVEP at points $$\lambda \in \sigma_{w}(M_{0}) \backslash {\sigma_{SF_{+}}}(A)$$ and B * has SVEP at points $$\mu \in  \sigma _{w}(M_{0}) \backslash \sigma_{SF_{-}}(B)$$, then $$\sigma (M_{C}) \backslash \sigma_{w}(M_{C}) = \pi_{0}(M_{C})$$. Here the hypothesis that λ ∈ π0(M C ) are poles of the resolvent of A can not be replaced by the hypothesis $$\lambda \in \pi_{0}(A)$$ are poles of the resolvent of A. For an operator $$T \in B(\chi)$$, let $$\pi_{0}^{a}(T)= \{ \lambda : \lambda \in\,\rm{iso}\, \sigma_a(T), 0 < \, \rm{dim}\,(T - \lambda)^{-1}(0)< \infty \}$$. We prove that if A* and B* have SVEP, A is polaroid on π a 0(M C) and B is polaroid on π a 0(B), then $$\sigma_a (M_C)\backslash \sigma_{aw}(M_C) = {\pi^{a}_{0}}(M_C)$$.
Keywords:Mathematics Subject Classification (2000)" target="_blank">Mathematics Subject Classification (2000)    Primary 47B47  47A10  47A11
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