Coecient Functional and Bohr-Rogosinski Phenomenon for Analytic functions involving Semigroup Generators Surya Giri and S. Sivaprasad Kumar

2025-04-29 0 0 391.01KB 15 页 10玖币
侵权投诉
Coefficient Functional and Bohr-Rogosinski Phenomenon for
Analytic functions involving Semigroup Generators
Surya Giri and S. Sivaprasad Kumar
Abstract
This paper examines the coefficient problems for the class of semigroup generators, a topic in complex
dynamics that has recently been studied in context of geometric function theory. Further, sharp bounds
of coefficient functional such as second order Hankel determinant, third order Toeplitz and Hermitian-
Toeplitz determinants are derived. Additionally, the sharp growth estimates and the bounds of difference
of successive coefficients are determined, which are used to prove the Bohr and the Bohr- Rogosinski
phenomenon for the class of semigroup generators.
Keywords: Holomorphic generators; Hankel determinant; Toeplitz determinant; Zalcman functional; Succes-
sive coefficient difference; Bohr and Bohr-Rogosinski radius.
AMS Subject Classification: 30C45, 30C50, 30C55, 47H20, 37L05.
1 Introduction
Let Hbe the class of holomorphic functions in the unit disk Dand A⊂ H containing functions of the form
f(z) = z+
X
n=2
anzn.(1.1)
By B, we denote the class of holomorphic self mappings from Dto D. A family {ut(z)}t0⊂ B is called a one
parameter continuous semigroup if (i) limt0ut(z) = z, (ii)ut+s(z) = ut(z)us(z), and (iii) limtsut(z) =
us(z) for each zDhold.
Berkson and Porta [3] showed that each one parameter semigroup is locally differentiable in parameter
t0 and moreover, if
lim
t0
zut(z)
t=f(z),
which is a holomorphic function, then ut(z) is the solution of the the Cauchy problem
ut(z)
t +f(ut(z)) = 0, u0(z) = z.
The function fis called the infinitesimal (holomorphic) generator of semigroup {ut(z)}⊂B. The class of all
holomorphic generators is denoted by G.Also, note that each element of {ut(z)}generated by f∈ H(D,C)
is univalent function while fis not necessarily univalent [13]. Different analytic criteria are available to show
that a function is semigroup generator [3, 37, 6]. Berkson and Porta [3] proved:
Theorem 1.1. The following assertions are equivalent:
(a)f∈ G;
(b)f(z)=(zσ)(1 z¯σ)p(z)with some σDand p∈ H,Re(p(z)) 0.
1
arXiv:2210.13166v1 [math.CV] 24 Oct 2022
The point σD:= {zC:|z| ≤ 1}is unique and called the Denjoy–Wolff point of the semigroup
generated by f(z). By Denjoy-Wolff theorem [13, 37, 36] for continuous semigroup, limt→∞ u(t, z) = σif
the semigroup generated by fis neither an elliptic automorphism of Dnor an identity map for at least one
t[0,). We denote the class of infinitesimal generators with Denjoy-Wolff point σby G[σ].For σ= 0, we
obtain the following subclass
G[0] = {f∈ G :f(z) = zp(z),Re p(z)0}.
Bracci et al. [7] considered the class G0=G[0]A. In the study of non-autonomous problem such as Loewner
theory, the class G0plays a significant role [8, 12]. Various subclasses of G0are considered with parameter,
which is also called filtration. For instance, the class
Aβ=f∈ A : Re βf(z)
z+ (1 β)f0(z)>0, β [0,1](1.2)
is a subclass of G0.In [7], the authors proved that Aβ1(Aβ2(G0for 0 β1< β2<1 and whenever
f∈ Aβ,
Re f(z)
zZ1
0
1t1β
1 + t1βdt.
Clearly, when β= 0, the class Aβreduces to the class R:= {f∈ A : Re f0(z)>0},which is called the
class of bounded turning functions. It can be easily seen that R⊂G0and each f∈ R satisfies the Noshiro-
Warshawski condition [12], thus every member of Rgenerates a semigroup that is univalent. Elin et al. [14]
solved the radii problems for the class Aβ. They found the radii r(0,1) for f∈ Aβsuch that f(rz)/r
belong to the class of starlike functions, denoted by S, and some other subclasses of starlike functions. This
problem arises from the fact that neither S⊂ Aβnor Aβ⊂ S. Generalizing this work, Giri and Kumar
[16] obtained rsuch that f(rz)/r belong to the class of Ma-Minda starlike functions.
Coefficient problems, growth estimates and others were still open for the class Aβ. In this paper, we focus
on these problems. We find the bound of nth coefficient of f∈ Aβand coefficient functional such as second
Hankel determinant, third order Toeplitz and Hermitian Toeplitz determinant and Zalcman functional.
Later, Bohr and Bohr-Rogosinski phenomenon with growth estimates are also discussed for this class.
In 1914, Bohr [5] proved that, if ω(z) = P
n=0 cnzn∈ B, then P
n=0|cn|rn1 for all zDwith
|z|=r1/3.The constant 1/3 is known as Bohr radius. This inequality was first derived by Bohr for
r1/6 and sharpened independently to r1/3 by Wiener, Riesz, and Schur. In recent years, a lot of
study have been carried out on the Bohr inequality for functions, which map Donto other domains, say Ω
[4, 15]. Different generalizations of the Bohr inequality are taken into consideration [39, 27]. We say that
Definition 1.2. The class Aβsatisfies the Bohr phenomenon if there exists rbsuch that
|z|+
X
n=2|an||z|nd(f(0), ∂f(Ω))
holds in |z|=rrb,where f(Ω) is the boundary of image domain of Dunder fand ddenotes the
Euclidean distance between f(0) and f(Ω).
For m= 1, Muhanna [32] showed that the Bohr phenomenon holds for the class of univalent functions
and the class of convex functions, when |z|=r322 and |z|=r1/3 respectively. We refer to the
survey article [31] for further details on this topic. There is also the concept of Rogosinski radius along with
the Bohr radius, although a little is known about Rogosinski radius in comparison to Bohr radius [17, 22, 35].
It says that, if ω(z) = P
n=0 cnzn∈ B, then
N1
X
n=0 |cn||z|n1 (NN)
in the disk |z|=r1/2.The radius 1/2 is called the Rogosinski radius. Kayumov et al. [18] considered
the following expression
Rf
N(z) := |f(z)|+
X
n=N|an||z|n
2
and found the radius rNsuch that Rf
N(z)1 in |z|=rrNfor the Ces´aro operators on the space of
bounded analytic functions. Here, we say that:
Definition 1.3. The class Aβsatisfies the Bohr-Rogosinski phenomenon if there exist rNsuch that
|f(zm)|+
X
n=N|an||z|nd(f(0), ∂f(Ω))
holds in |z|=rrN.
Section 5 is devoted to find the rband rNfor the class Aβ.
For f(z) = z+P
n=2 anzn∈ A, the mth Hankel, Toeplitz and Hermitian Toeplitz determinant for m1
and n0 are respectively given by
Hm(n)(f) =
anan+1 ··· an+m1
an+1 an+2 ··· an+m
.
.
..
.
..
.
..
.
.
an+m1an+m··· an+2m2
,
Tm(n)(f) =
anan+1 ··· an+m1
an+1 an··· an+m2
.
.
..
.
..
.
..
.
.
an+m1an+m2··· an
,(1.3)
Tm,n(f) =
anan+1 ··· an+m1
¯an+1 an··· an+m2
.
.
..
.
..
.
..
.
.
¯an+m1¯an+m2··· an
,(1.4)
where ¯an=an. Toeplitz matrices have constant entries along their diagonals, while Hankel matrices have
constant entries along their reverse diagonals. In particular,
H2(n)(f) = anan+2 a2
n+1, T3(1)(f)=12a2
2+ 2a2
2a3a2
3
and T3,1(f) = 1 2|a2|2+ 2 Re(a2
2¯a3)− |a3|2.Finding the sharp bound of |H2(2)(f)|for the class Sand its
subclasses has always been the focus of many researchers. Although, investigations concerning Toeplitz and
Hermitian Toeplitz are recently introduced in [2, 11], a summary of some of the more significant results is
given in [38]. For more work in this direction (see [21, 20, 24, 33]).
In 1999, Ma [28] proposed a conjecture for f(z) = z+P
n=2 anzn∈ S that
|Jm,n|:= |anaman+m1| ≤ (m1)(n1).
They proved this conjecture for the class of starlike functions and univalent functions with real coefficients. It
is also called generalized Zalcman conjecture as it generalizes the Zalcman conjecture |a2
na2n1| ≤ (2n1)2
for f∈ S. Recently, bound of |J2,3|are obtained for various subclasses of A[1, 10]. In section 2 and 3, we
obtain the sharp bound of |H2(2)(f)|,|T3(1)(f)|and |J2,3(f)|for f∈ Aβ.
2 Hankel Determinant and Zalcman Functional
Theorem 2.1. If f∈ Aβis of the form (1.1), then
|an| ≤ 2
nβ(n1).(2.1)
Further, this inequality is sharp for each n.
3
摘要:

CoecientFunctionalandBohr-RogosinskiPhenomenonforAnalyticfunctionsinvolvingSemigroupGeneratorsSuryaGiriandS.SivaprasadKumarAbstractThispaperexaminesthecoecientproblemsfortheclassofsemigroupgenerators,atopicincomplexdynamicsthathasrecentlybeenstudiedincontextofgeometricfunctiontheory.Further,sharpb...

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