Characterization of bounded generalized Hilbert operators on Hardy spaces for p greater than 2
Establish a complete characterization of the symbols g for which the generalized Hilbert operator H_g, defined by H_g(f)(z)=\int_0^1 f(t)g'(tz)\,dt, is bounded on the Hardy space H^p when 2<p<\infty.
References
The boundedness of $H$ on $Hp$ is well understood when $1<p\leq 2$, whereas the case $2<p<\infty$ remains open. More precisely, the condition $g\in\Lambda\left(p,\frac{1}{p}\right)$ is necessary for the boundedness of $H$ on $Hp$ whenever $1<p<\infty$, and it is also sufficient when $1<p\leq 2$ cite[Theorem 1]{GaGiPeSis}. For $2<p<\infty$, however, this condition is no longer sufficient cite[Theorem~3.5 and Corollary~3.6]{GuoTang2026}, and no complete characterization is currently known.
Looking at Theorem \ref{summing up}, Theorem \ref{summing up2}, Theorem \ref{Rhaly Hardy} and Theorem \ref{Hg Hardy} it is natural to wander what happens with case $\mathcal R_{\eta}: Hp \to Hq,\,\, 2<p\leq q <\infty.$
Additionally, the authors proposed an unresolved conjecture stating that the equality
|\mathcal{H}b|{H{p}\to H{p} = B\Big(\frac{1}{p},~b+1-\frac{1}{p}\Big)
holds for $b \geq 0$ and $1 < p < \infty$.