Abstract
AbstractLet $$\mathbb {D}$$
D
denote the unit disc in $$\mathbb {C}$$
C
. We define the generalized Cesàro operator as follows: $$\begin{aligned} C_{\omega }(f)(z)=\int _0^1 f(tz)\left( \frac{1}{z}\int _0^z B^{\omega }_t(u)\,\textrm{d}u\right) \,\omega (t)\textrm{d}t, \end{aligned}$$
C
ω
(
f
)
(
z
)
=
∫
0
1
f
(
t
z
)
1
z
∫
0
z
B
t
ω
(
u
)
d
u
ω
(
t
)
d
t
,
where $$\{B^{\omega }_\zeta \}_{\zeta \in \mathbb {D}}$$
{
B
ζ
ω
}
ζ
∈
D
are the reproducing kernels of the Bergman space $$A^{2}_{\omega }$$
A
ω
2
induced by a radial weight $$\omega $$
ω
in the unit disc $$\mathbb {D}$$
D
. We study the action of the operator $$C_{\omega }$$
C
ω
on weighted Hardy spaces of analytic functions $$\mathcal {H}_{\gamma }$$
H
γ
, $$\gamma >0$$
γ
>
0
and on general weighted Bergman spaces $$A^{2}_{\mu }$$
A
μ
2
.
Funder
Ministerio de Ciencia e Innovación
Junta de Andalucía
Publisher
Springer Science and Business Media LLC