Subnormality for arbitrary powers of 2-variable weighted shifts whose restrictions to a large invariant subspace are tensor products

preprint2011arXivOpen access

Abstract

The Lifting Problem for Commuting Subnormals (LPCS) asks for necessary and sufficient conditions for a pair of subnormal operators on Hilbert space to admit commuting normal extensions. \ We study LPCS within the class of commuting 2-variable weighted shifts T≡(T1,T2)\mathbf{T} \equiv (T_1,T_2) with subnormal components T1T_1 and T2T_2, acting on the Hilbert space ℓ2(Z+2)\ell ^2(\mathbb{Z}^2_+) with canonical orthonormal basis {e(k1,k2)}k1,k2≥0\{e_{(k_1,k_2)}\}_{k_1,k_2 \geq 0} . \ The \textit{core} of a commuting 2-variable weighted shift T\mathbf{T}, c(T)c(\mathbf{T}), is the restriction of T\mathbf{T} to the invariant subspace generated by all vectors e(k1,k2)e_{(k_1,k_2)} with k1,k2≥1k_1,k_2 \geq 1; we say that c(T)c(\mathbf{T}) is of \textit{tensor form} if it is unitarily equivalent to a shift of the form (I⊗Wα,Wβ⊗I)(I \otimes W_α, W_β\otimes I), where WαW_α and WβW_β are subnormal unilateral weighted shifts. \ Given a 2-variable weighted shift T\mathbf{T} whose core is of tensor form, we prove that LPCS is solvable for T\mathbf{T} if and only if LPCS is solvable for any power T(m,n):=(T1m,T2n)\mathbf{T}^{(m,n)}:=(T^m_1,T^n_2) (m,n≥1m,n\geq 1). \

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