Abstract

Let b(z)=∏n=1∞−αˉn∣αn∣z−αn1−αˉnzb(z) = \prod_{n=1}^\infty \frac{-\barα_n}{|α_n|} \frac{z - α_n}{1 - \barα_n z}, where ∑n=1∞(1−∣αn∣)<∞\sum_{n=1}^\infty (1 - |α_n|) <\infty, be the Blaschke product with zeros at αn∈D∖{0}α_n \in \mathbb{D} \setminus \{0\}. Then $\cls = \vee_{n=1}^\infty \big(z^n H^2(\mathbb{D})\big) \otimes \big(\prod_{k=n}^\infty \frac{-\barα_n}{|α_n|} \frac{z - α_n}{1 - \barα_n z} H^2(\mathbb{D})\big)$ is a joint (Mz1,Mz2)(M_{z_1}, M_{z_2}) invariant subspace of the Hardy space H2(D2)≅H2(D)⊗H2(D)H^2(\mathbb{D}^2) \cong H^2(\mathbb{D}) \otimes H^2(\mathbb{D}). This class of subspaces was originally introduced by Rudin in the context of infinite cardinality of generating sets of shift invariant subspaces of H2(D2)H^2(\mathbb{D}^2). \noindent In this paper we prove that for a Rudin invariant subspace $\cls$ of H2(D2)H^2(\mathbb{D}^2), the cross commutator $[(P_{\cls} M_{z_1}|_{\cls})^*, M_{z_2}|_{\cls}] = (P_{\cls} M_{z_1} |_{\cls})^* (M_{z_2}|_{\cls}) - (M_{z_2}|_{\cls}) (P_{\cls} M_{z_1}|_{\cls})^*$ is not compact. Consequently, Rudin's invariant subspaces are both infinitely generated and not essentially doubly commuting.

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