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A Hankel matrix acting on spaces of analytic functions

Abstract

If μ\mu is a positive Borel measure on the interval [0,1)[0, 1) we let Hμ\mathcal H_\mu be the Hankel matrix Hμ=(μn,k)n,k0\mathcal H_\mu =(\mu _{n, k})_{n,k\ge 0} with entries μn,k=μn+k\mu _{n, k}=\mu _{n+k}, where, for n=0,1,2,n\,=\,0, 1, 2, \dots , μn\mu_n denotes the moment of order nn of μ\mu . This matrix induces formally the operator Hμ(f)(z)=n=0(k=0μn,kak)zn\mathcal{H}_\mu (f)(z)= \sum_{n=0}^{\infty}\left(\sum_{k=0}^{\infty} \mu_{n,k}{a_k}\right)z^n on the space of all analytic functions f(z)=k=0akzkf(z)=\sum_{k=0}^\infty a_kz^k, in the unit disc D\mathbb D . This is a natural generalization of the classical Hilbert operator. In this paper we improve the results obtained in some recent papers concerning the action of the operators HμH_\mu on Hardy spaces and on M\"obius invariant spaces.Comment: arXiv admin note: text overlap with arXiv:1612.0830

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