Abstract
AbstractLet $${\mathbb {D}}$$
D
be the unit disc in $${\mathbb {C}}$$
C
. If $$\mu $$
μ
is a finite positive Borel measure on the interval [0, 1) and f is an analytic function in $${\mathbb {D}}$$
D
, $$f(z)=\sum _{n=0}^\infty a_nz^n$$
f
(
z
)
=
∑
n
=
0
∞
a
n
z
n
($$z\in {\mathbb {D}}$$
z
∈
D
), we define $$\begin{aligned} {\mathcal {C}}_\mu (f)(z)= \sum _{n=0}^\infty \mu _n\left( \sum _{k=0}^na_k\right) z^n,\quad z\in {\mathbb {D}}, \end{aligned}$$
C
μ
(
f
)
(
z
)
=
∑
n
=
0
∞
μ
n
∑
k
=
0
n
a
k
z
n
,
z
∈
D
,
where, for $$n\ge 0$$
n
≥
0
, $$\mu _n$$
μ
n
denotes the n-th moment of the measure $$\mu $$
μ
, that is, $$\mu _n=\int _{[0, 1)}t^nd\mu (t).$$
μ
n
=
∫
[
0
,
1
)
t
n
d
μ
(
t
)
.
In this way, $${\mathcal {C}}_\mu $$
C
μ
becomes a linear operator defined on the space $${\mathrm{Hol}}({\mathbb {D}})$$
Hol
(
D
)
of all analytic functions in $${\mathbb {D}}$$
D
. We study the action of the operators $${\mathcal {C}}_\mu $$
C
μ
on distinct spaces of analytic functions in $${\mathbb {D}}$$
D
, such as the Hardy spaces $$H^p$$
H
p
, the weighted Bergman spaces $$A^p_\alpha $$
A
α
p
, BMOA, and the Bloch space $${\mathcal {B}}$$
B
.
Funder
Ministerio de Economía y Competitividad
Consejería de Economía, Innovación, Ciencia y Empleo, Junta de Andalucía
Publisher
Springer Science and Business Media LLC
Subject
Mathematical Physics,Algebra and Number Theory,Analysis
Cited by
14 articles.
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