A Derivative-Hilbert operator acting on Hardy spaces
Let $\mu$ be a positive Borel measure on the interval [0,1). The Hankel matrix $\mathcal{H}_\mu= (\mu_{n,k})_{n,k\geq0}$ with entries $\mu_{n,k}= \mu_{n+k}$, where $\mu_n=\int_{ [0,1)}t^nd\mu(t)$, induces formally the operator $$\mathcal{DH}_\mu(f)(z)=\sum_{n=0}^\infty (\sum_{k=0}^\infty \mu_{n,k}a_...
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Zusammenfassung: | Let $\mu$ be a positive Borel measure on the interval [0,1). The Hankel
matrix $\mathcal{H}_\mu= (\mu_{n,k})_{n,k\geq0}$ with entries $\mu_{n,k}=
\mu_{n+k}$, where $\mu_n=\int_{ [0,1)}t^nd\mu(t)$, induces formally the
operator $$\mathcal{DH}_\mu(f)(z)=\sum_{n=0}^\infty (\sum_{k=0}^\infty
\mu_{n,k}a_k)(n+1)z^n$$ on the space of all analytic function $f(z)=\sum_{k=0}^
\infty a_k z^n$ in the unit disc $\mathbb{D}$. We characterize those positive
Borel measures on $[0,1)$ such that $\mathcal{DH}_\mu(f)(z)= \int_{[0,1)}
\frac{f(t)}{{(1-tz)^2}} d\mu(t)$ for all in Hardy spaces $H^p(0 |
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DOI: | 10.48550/arxiv.2206.12024 |