Next Article in Journal
Steganographic Method in Selected Areas of the Stego-Carrier in the Spatial Domain
Next Article in Special Issue
Complex-Variable Dynamic System of Layla and Majnun Model with Analytic Solutions
Previous Article in Journal
Generalized AB-Fractional Operator Inclusions of Hermite–Hadamard’s Type via Fractional Integration
Previous Article in Special Issue
Applications of Gegenbauer Polynomials for Subfamilies of Bi-Univalent Functions Involving a Borel Distribution-Type Mittag-Leffler Function
 
 
Font Type:
Arial Georgia Verdana
Font Size:
Aa Aa Aa
Line Spacing:
Column Width:
Background:
Article

Univalence and Starlikeness of Certain Classes of Analytic Functions

1
Department of Mathematics, Imam Abdulrahman Bin Faisal University, P.O. Box 1982, Dammam 31441, Saudi Arabia
2
Department of Mathematics, Faculty of Civil Engineering, Bulevar Kralja Aleksandra 73, 11000 Belgrade, Serbia
*
Author to whom correspondence should be addressed.
Symmetry 2023, 15(5), 1014; https://doi.org/10.3390/sym15051014
Submission received: 24 March 2023 / Revised: 7 April 2023 / Accepted: 12 April 2023 / Published: 2 May 2023
(This article belongs to the Special Issue Symmetry in Mathematical Functional Equations)

Abstract

:
For the analytic functions ϕ ( ζ ) = ζ + k = n ϕ k ζ k in the unit disk O , we calculate the values of n and α , where the condition 1 + ζ ϕ ( ζ ) / ϕ ( ζ ) > α or 1 + ζ ϕ ( ζ ) / ϕ ( ζ ) < 1 + α / 2 yields univalence and starlikeness. Conditions imply ϕ in the class where all normalized analytic functions U , with ζ / ϕ ( ζ ) 2 ϕ ( ζ ) 1 < 1 are obtained. Recent findings are gained, and unique cases are demonstrated. The generalization of the Jack lemma serves the proof of the main result and that our methodology is based on the idea of subordination.

1. Introduction

Symmetry in the open unit disk O : = { ζ C : | ζ | < 1 } can refer to several different types of symmetry, including rotational symmetry, reflection symmetry, and inversion symmetry. Inversion symmetry refers to the property that the open unit disk looks the same when inverted with respect to a certain point. The open unit disk has inversion symmetry with respect to its center (the origin), because inverting any complex number ζ in the disk with respect to the origin gives the complex number 1 / ζ , which is also in the disk. Generally, the open unit disk has a rich set of symmetries, which can be useful in a variety of mathematical and geometric contexts. In this effort we aim to explore more geometric properties in this symmetry domain.
A function is said to be starlike if it maps a disk in the complex plane onto a shape that is itself star-shaped with respect to some fixed point in the disk. In other words, a function is starlike if its image under a suitable scaling and rotation is contained in a star-shaped domain, where the star-shaped domain is obtained by connecting the fixed point to all other points in the domain using straight line segments. Another term for a starlike function is a convex function. Both univalent functions and starlike functions are important subclasses of analytic functions in complex analysis, and they have many interesting properties and applications. For example, univalent functions are often used in geometric function theory to study conformal mappings and the Riemann mapping theorem, while starlike functions are used in geometric function theory and mathematical physics to model phenomena such as electrostatics [1,2] and fluid flow [3,4].
Ozaki [5] presented a condition on a normalized class of analytic function to univalently satisfy thw real inequality
1 + ζ ϕ ( ζ ) ϕ ( ζ ) < 3 2 .
Consequently, the above inequality is used to show the convexity and close to convex properties in one direction [6,7], respectively. Currently, as an application of the Ozaki inequality, many classes of analytic functions involve polynomials, special functions and different types of operators of the normalized class are investigated. For example, the starlikeness property is studied in [8,9,10]; the convex property is checked in [11,12,13] and the close to convex property is realized in [14,15].
In this effort, we proceed with the investigation on univalency and starlikeness of the normalized class. We shall deal with the U class such that the inequality
ζ ϕ ( ζ ) 2 ϕ ( ζ ) 1 < 1
is satisfied. Some recent results are obtained and special cases are illustrated. Our methodology is based on the concept of subordination and the proof is given by the generalization of Jack lemma.
The effort is organized as follows: Section 2 deals with the general information that can be utilized in the proof. Section 3 shows our results and their consequences. Section 4 is the conclusion of this work.

2. Information

Let A n , n 2 denote the set of all analytic functions ϕ in O taking the power series
ϕ ( ζ ) = ζ + ϕ n ζ n + ϕ n + 1 ζ n + 1 +
with A 2 = A . Let S be its subclass of univalent functions and S S be the class of all starlike univalent functions. Every ϕ S characterized analytically by
Re ζ ϕ ( ζ ) ϕ ( ζ ) > 0 , ζ O .
A function ϕ S is called convex ( C ) if and only if ζ ϕ S (see [16]). Let U be the set of all ϕ A achieving the inequality | U ϕ ( ζ ) | < 1 for ζ O , where
U ϕ ( ζ ) = ζ ϕ ( ζ ) 2 ϕ ( ζ ) 1 .
For example of functions in U ϕ ( ζ ) , one can realize that the following set:
S Z = ζ , ζ ( 1 ± ζ ) 2 , ζ 1 ± ζ , ζ 1 ± ζ 2 , ζ 1 ± ζ + ζ 2
belongs to U . Clearly,
κ ( ζ ) = ζ ( 1 ζ ) 2 U S .
Moreover, it recognized the following inclusion [17]:
S Z S S .
Basic properties of the class U were studied in [18]. In recent years, the class U has received a lot of attention, for instance in the works of [19,20,21,22,23,24,25,26,27,28,29,30,31,32,33,34,35,36,37].
Recall that an analytic function ϕ is subordinate to the analytic function ψ symbolized by ϕ ( ζ ) ψ ( ζ ) ), if there exists an analytic self-map ω of O with ω ( 0 ) = 0 satisfying
ϕ ( ζ ) = ψ ( ω ( ζ ) ) .
In the foregoing discussion, for ϕ A n , n 2 we determine values of n such that the condition
Re 1 + ζ ϕ ( ζ ) ϕ ( ζ ) > α
or
Re 1 + ζ ϕ ( ζ ) ϕ ( ζ ) < 1 + α / 2
implies univalence and starlikeness. Additionally, conditions implying ϕ in the class U were obtained. For the analytic functions ϕ A 2 and α = 1 , the condition for starlikeness were determined for the class Re 1 + ζ ϕ ( ζ ) / ϕ ( ζ ) < 3 / 2 in [19].
We request the next result.
Lemma 1 
([20] (p. 19)). Assume that ζ 0 O and r 0 = | ζ 0 | . Moreover, assume that
ϕ ( ζ ) = ϕ n ζ n + ϕ n + 1 ζ n + 1 +
is analytic on O r 0 { ζ 0 } with ϕ ( ζ ) 0 and n 1 . If
| ϕ ( ζ 0 ) | = max { | ϕ ( ζ ) | : ζ O ¯ r 0 } ,
then there exists an m n such that
  • ζ 0 ϕ ( ζ 0 ) ϕ ( ζ 0 ) = m , and
  • ζ 0 ϕ ( ζ 0 ) ϕ ( ζ 0 ) + 1 m .

3. Main Results

In this section, we illustrate our main results. These results describe the univalency property via the behavior of bounded functions. Let r 0 be the largest radius such that ϕ ( ζ ) maps the circle | ζ | = r 0 inside the unit disk O . Then, the bounded turning class of ϕ ( ζ ) is the smallest non-negative number α such that ϕ ( ζ ) maps the circle | ζ | = r inside the sector | arg ζ | < α for all r with 0 < r r 0 .
In other words, the bounded turning class measures the maximum amount of turning that the function exhibits on the unit circle, as we move outward from the origin. The bounded turning class is an important concept in the theory of univalent functions, and it has been extensively studied in the literature. Properties of the bounded turning class are closely related to the geometric properties of univalent functions, such as the distortion theorem and the Koebe one-quarter theorem. For example, let
ϕ ( ζ ) = ζ ( 1 ζ ) , ζ O
then the basic condition for bounded turning is that (see Figure 1)
ζ / ( 1 ζ ) > 0 , ζ O .
Theorem 1. 
Let α > 0 and ϕ A n satisfy the condition
Re 1 + ζ ϕ ( ζ ) ϕ ( ζ ) < 1 + α 2 , ζ O
(a) 
If n 1 + α , and ϕ ( ζ ) / ζ 0 , then Re ( ϕ ( ζ ) ) > 0 , ζ O .
(b) 
If n 1 + α , and ϕ ( ζ ) / ζ 0 , then
ζ ϕ ( ζ ) / ϕ ( ζ ) ( 1 ζ ) / ( 1 a ζ ) , ζ O , a = 1 / ( 1 + α ) .
(c) 
If n 5 + α and ϕ ( ζ ) / ζ 0 , then ϕ U .
Proof. 
(a)
First, prove that ϕ ( ζ ) 0 for all ζ O and ζ 0 (since ϕ ( 0 ) = 1 ). If there exists ζ 1 , 0 < | ζ 1 | < 1 and
ϕ ( ζ ) = ( ζ ζ 1 ) m 1 ψ ( ζ ) ,
where m 1 1 and ψ is analytic in O and ψ ( ζ 1 ) 0 , then
1 + ζ ϕ ( ζ ) ϕ ( ζ ) = 1 + m 1 ζ ζ ζ 1 + ζ ψ ( ζ ) ψ ( ζ ) .
Thus, 1 + ζ ϕ ( ζ ) / ϕ ( ζ ) when ζ ζ 1 , which is a contradiction to (1).
Let
ϕ ( ζ ) = 1 ω ( ζ ) α n 1 ,
where 0 < α / ( n 1 ) 1 .
Since previous ϕ ( ζ ) 0 for all ζ O , then ω ( ζ ) = b n 1 ζ n 1 + is analytic in O with ω ( 0 ) = 0 . Furthermore, it follows from (2) that
1 + ζ ϕ ( ζ ) ϕ ( ζ ) = 1 α ζ ω ( ζ ) ( n 1 ) ( 1 ω ( ζ ) ) .
Consider that ζ 0 O , such that
max | ζ | | ζ 0 | | ω ( ζ ) | = | ω ( ζ 0 ) | = 1 .
In view of Lemma 1, we have
ζ 0 ω ( ζ 0 ) = k ω ( ζ 0 ) ; ( k n 1 ; ω ( ζ 0 ) = e i θ ; θ R ) ,
thus
Re 1 + ζ 0 ϕ ( ζ 0 ) ϕ ( ζ 0 ) = 1 α n 1 Re k e i θ 1 e i θ .
Hence, the following is obtained
Re 1 + ζ 0 ϕ ( ζ 0 ) ϕ ( ζ 0 ) = 1 + k α 2 ( n 1 ) 1 + α 2 ,
which is a contradiction to (1). It means that | ω ( ζ ) | < 1 , ζ O , and from (2) finally leads to
| arg ( ϕ ( ζ ) ) | = α n 1 | arg ( ( 1 ω ( ζ ) ) | < α ( n 1 ) π 2 π 2 ,
where n 1 + α , which implies Re ( ϕ ( ζ ) ) > 0 , ζ O ,
(b)
Define a function ω by
ζ ϕ ( ζ ) ϕ ( ζ ) = 1 ω ( ζ ) 1 a ω ( ζ ) ,
where a = 1 / ( 1 + α ) , then ω ( ζ ) = c n 1 ζ n 1 + is analytic in O . Additionally, suppose that there is a point ζ 0 O , such that
max | ζ | | ζ 0 | | ω ( ζ ) | = | ω ( ζ 0 ) | = 1 .
Then by applying Lemma 1, the following is acquired
ζ 0 ω ( ζ 0 ) = k ω ( ζ 0 ) ; ( k n 1 ; ω ( ζ 0 ) = e i θ ; θ R ) .
From (3), logarithmic differentiation, yields
Re 1 + ζ 0 ϕ ( ζ 0 ) ϕ ( ζ 0 ) = Re a ζ 0 ω ( ζ 0 ) 1 a ω ( ζ 0 ) ζ 0 ω ( ζ 0 ) 1 ω ( ζ 0 ) + 1 ω ( ζ 0 ) 1 a ω ( ζ 0 ) = Re a k e i θ 1 a e i θ k e i θ 1 e i θ + 1 e i θ 1 a e i θ = 1 + a 2 φ ( t ) , t = c o s θ
where
φ ( t ) = k ( 1 a ) + 2 ( 1 t ) 1 2 a t + a 2 , 1 t 1 .
Since α > 0 , 0 < a = 1 / ( 1 + α ) < 1 and n 1 + α , then n a 1 0 . Thus,
φ ( t ) = 2 ( 1 a ) ( k + 1 ) a 1 ( 1 2 a t + a 2 ) 2 2 ( 1 a ) n a 1 ( 1 2 a t + a 2 ) 2 0 ,
which implies that the function φ is a non-decreasing function and
φ ( t ) φ ( 1 ) = ( n 1 ) ( 1 a ) + 4 ( 1 + a ) 2 .
Hence, the previous relation shows that
Re 1 + ζ 0 ϕ ( ζ 0 ) ϕ ( ζ 0 ) ( n 1 ) ( 1 a ) + 4 2 ( 1 + a ) 1 + α 2 ,
which is a contradiction to (1). From that | ω ( ζ ) | < 1 , ζ O is obtained and (3) shows that the statement of the theorem is valid.
(c)
Let
ζ ϕ ( ζ ) 2 ϕ ( ζ ) 1 = ω ( ζ ) .
Then, ω ( ζ ) = d n 1 ζ n 1 + is analytic in O . Additionally, from (4) and after logarithmic differentiation, it calculates to
1 + ζ ϕ ( ζ ) ϕ ( ζ ) = ζ ω ( ζ ) 1 + ω ( ζ ) + 2 ζ ϕ ( ζ ) ϕ ( ζ ) 1 .
Relation (5) and the condition (1), lead to
Re ζ ω ( ζ ) 1 + ω ( ζ ) + 2 ζ ϕ ( ζ ) ϕ ( ζ ) 1 < 1 + α 2 .
Additionally, note that if n 5 + α , then n 1 + α . Hence, (b) shows that
ζ ϕ ( ζ ) ϕ ( ζ ) 1 ζ 1 a ζ ,
where a = 1 / ( 1 + α ) , which implies
Re ζ ϕ ( ζ ) ϕ ( ζ ) > 0 .
Thus, (6) becomes
Re ζ ω ( ζ ) 1 + ω ( ζ ) 1 < 1 + α 2 2 Re ζ ϕ ( ζ ) ϕ ( ζ ) < 1 + α 2 .
Now suppose that there exists a point ζ 0 O , such that | ω ( ζ 0 ) | = 1 . Then, by applying Lemma 1, the following is obtained:
ζ 0 ω ( ζ 0 ) = k ω ( ζ 0 ) ; ( k n 1 ; ω ( ζ 0 ) = e i θ ; θ R ) ,
thus
Re ζ 0 ω ( ζ 0 ) 1 + ω ( ζ 0 ) 1 = Re k e i θ 1 + e i θ 1 = k 2 1 .
Hence,
Re ζ 0 ω ( ζ 0 ) ω ( ζ 0 ) 1 1 + α 2 ,
where k n 1 , and n 5 + α , which is a contradiction to (1). It means that | ω ( ζ ) | < 1 , ζ O . Moreover, (4) shows that
ζ ϕ ( ζ ) 2 ϕ ( ζ ) 1 < 1 , ζ O
which concludes the desired ϕ U .
 □
For α = 1 , we have the next result.
Corollary 1. 
If ϕ A 2 satisfies the condition
Re 1 + ζ ϕ ( ζ ) ϕ ( ζ ) < 3 2 , ζ O ,
then
(a) 
Re ( ϕ ( ζ ) ) > 0 , ζ O .
(b) 
ζ ϕ ( ζ ) ϕ ( ζ ) 1 ζ 1 ζ / 2 .
These are the former results given in [19].
Theorem 2. 
Assume that α 0 and ϕ A n , n 2 satisfy the condition
Re 1 + ζ ϕ ( ζ ) ϕ ( ζ ) > α , ζ O .
(a) 
If n 2 α + 3 , then Re ( ϕ ( ζ ) ) > 0 , ζ O .
(b) 
If n 2 α + 2 , and ϕ ( ζ ) / ζ 0 , then ζ ϕ ( ζ ) / ϕ ( ζ ) 1 / ( 1 ζ )
(c) 
For every n N , and n > 2 , there exist ϕ A n and ϕ U such that (8) is not satisfied, or equivalently
Re 1 + ζ ϕ ( ζ ) ϕ ( ζ ) ,
where ζ O , ζ is real, and ζ 1 .
(d) 
For n = 2 , there exists ϕ A 2 such that (8) is satisfied for every α > 0 , but ϕ U .
Proof. 
(a)
Let
ϕ ( ζ ) = 1 1 ω ( ζ ) 2 ( α + 1 ) n 1 ,
where 0 < 2 ( 1 + α ) / ( n 1 ) 1 . Similarly, as in the proof of the previous theorem, ϕ ( ζ ) 0 for all ζ O , which implies that ω ( ζ ) = b n 1 ζ n 1 + is analytic in O with ω ( 0 ) = 0 . Additionally, from (9) and after logarithmic differentiation, it yields
1 + ζ ϕ ( ζ ) ϕ ( ζ ) = 1 + 2 ( α + 1 ) ( ζ ω ( ζ ) ) ( n 1 ) ( 1 ω ( ζ ) ) .
Suppose that there exists a point ζ 0 O , such that
max | ζ | | ζ 0 | | ω ( ζ ) | = | ω ( ζ 0 ) | = 1 .
Then, by applying Lemma 1, the following is acquired:
ζ 0 ω ( ζ 0 ) = k ω ( ζ 0 ) ; ( k n 1 ; ω ( ζ 0 ) = e i θ ; θ R ) .
Thus,
Re 1 + ζ 0 ϕ ( ζ 0 ) ϕ ( ζ 0 ) = 1 + 2 ( α + 1 ) n 1 Re k e i θ 1 e i θ = 1 k ( α + 1 ) n 1 α ,
which is a contradiction to (8). That implies | ω ( ζ ) | < 1 , ζ O . Furthermore, (9) shows that
| arg ( ϕ ( ζ ) ) | = 2 ( α + 1 ) n 1 | arg ( ( 1 ω ( ζ ) ) | < 2 ( α + 1 ) n 1 π 2 π 2 ,
where n 2 α + 3 . Hence, Re ( ϕ ( ζ ) ) > 0 , ζ O .
(b)
Define a function ω by
ζ ϕ ( ζ ) ϕ ( ζ ) = 1 1 ω ( ζ ) .
Then, ω ( ζ ) = c n 1 ζ n 1 + is analytic in O . Additionally, suppose that there exists a point ζ 0 O , such that
max | ζ | | ζ 0 | | ω ( ζ ) | = | ω ( ζ 0 ) | = 1 .
By applying Lemma 1,
ζ 0 ω ( ζ 0 ) = k ω ( ζ 0 ) ; ( k n 1 ; ω ( ζ 0 ) = e i θ ; θ R ) .
Therefore, (11) leads to
Re 1 + ζ 0 ϕ ( ζ 0 ) ϕ ( ζ 0 ) = Re ζ 0 ω ( ζ 0 ) 1 ω ( ζ 0 ) + 1 1 ω ( ζ 0 ) = Re k e i θ + 1 1 e i θ = 1 k 2 α ,
where
k 1 ( n 1 ) 1 = n 2 ( 2 α + 2 ) 2 = 2 α .
Which is a contradiction to (8). Thus, | ω ( ζ ) | < 1 , ζ O and (11) shows that the statement of the theorem is valid.
(c)
For n > 2 , let ϕ A n be defined by
ζ ϕ ( ζ ) = 1 + 1 n 2 ζ n 1 .
Since
ζ ϕ ( ζ ) 2 ϕ ( ζ ) 1 = | ζ n 1 | < 1 ,
then ϕ U . After logarithmic differentiation, the following is obtained:
1 + ζ ϕ ( ζ ) ϕ ( ζ ) = 1 ( n 1 ) ζ n 2 1 ζ n 2 2 ( n 1 ) ζ n 1 ( n 2 ) + ζ n 1 .
Thus, when ζ is real, ζ 1 and ζ O , we have
Re 1 + ζ ϕ ( ζ ) ϕ ( ζ ) .
(d)
Let ϕ A 2 be defined by ϕ ( ζ ) = ln ( 1 ζ ) . Then,
1 + ζ ϕ ( ζ ) ϕ ( ζ ) = 1 1 ζ ,
which implies that
Re 1 + ζ ϕ ( ζ ) ϕ ( ζ ) > 1 2 > α .
Since
ζ ϕ ( ζ ) 2 ϕ ( ζ ) 1 = ζ ln ( 1 ζ ) 2 1 1 ζ 1 ,
and ( 1 ζ ) ln 2 ( 1 ζ ) 0 when ζ O , ζ 1 is real, it follows that
ζ ϕ ( ζ ) 2 ϕ ( ζ ) 1 > 1 , ζ O .
Hence, ϕ U .
For α = 0 and α = 1 / 2 , Theorem 2 leads to the next corollaries.
Corollary 2. 
If ϕ A n satisfies the condition
Re 1 + ζ ϕ ( ζ ) ϕ ( ζ ) > 0 , ζ O ,
(a) 
Then, Re ( ϕ ( ζ ) ) > 0 , ζ O , whenever n 3 .
(b) 
Then, Re ζ ϕ ( ζ ) / ϕ ( ζ ) > 1 / 2 , ζ O , whenever n 2 and ϕ ( ζ ) / ζ 0 .
Remark 1. 
For the function ϕ ( ζ ) = ζ / ( 1 ζ ) A 2 , we have ϕ ( ζ ) = 1 / ( 1 ζ ) 2 and it has a non-positive real part in O , which means that the result (a) is the best possible. The result (b) is well-known.
Corollary 3. 
If ϕ A n satisfies the condition
Re 1 + ζ ϕ ( ζ ) ϕ ( ζ ) > 1 2 , ζ O .
(a) 
Then, Re ( ϕ ( ζ ) ) > 0 , ζ O , whenever n 4 .
(b) 
Then, Re ζ ϕ ( ζ ) / ϕ ( ζ ) > 1 / 2 , ζ O , whenever n 3 and ϕ ( ζ ) / ζ 0 .
Remark 2. 
The result (b) for n = 3 is given in ([20] (Theorem 2.6i, p. 68)).
Theorem 3. 
If α > 0 and ϕ A n satisfy the condition
ϕ ( ζ ) α , ζ O ,
then for n α + 1 , Re ϕ ( ζ ) > 0 , ζ O , that is, ϕ ( ζ ) 1 < 1 .
Proof. 
From (13) we have that
ζ ϕ ( ζ ) α | ζ | < α , ζ O .
Putting
ϕ ( ζ ) = 1 w ( ζ ) .
Then, w is analytic in O with w ( 0 ) = 0 , and we want to prove that | w ( ζ ) | < 1 , ζ O . If not, then by Lemma 1, there exists a point ζ 0 O such that
ζ 0 w ( ζ 0 ) = k w ( ζ 0 ) , k 1 , w ( ζ 0 ) = e i θ , θ R .
Now, by (15) we have
ζ 0 ϕ ( ζ 0 ) = ζ 0 w ( ζ 0 ) = k | w ( ζ 0 ) | n 1 α ,
which is a contradiction to (13). It means that | w ( ζ ) | < 1 and from (15) that | ϕ ( ζ ) 1 | < 1 , ζ O .  □
Remark 3. 
Since
ϕ ( ζ ) 1 = 0 ζ ϕ ( ζ ) d ζ
and | ϕ ( ζ ) | < α , then
| ϕ ( ζ ) 1 | = | 0 ζ ϕ ( ζ ) d ζ | < α | ζ | < 1
only if 0 < α 1 . However, from Theorem 3 it is true for all α > 0 with the condition n 1 + α . For example, if α = 2 , i . e . , | ϕ ( ζ ) | < 2 , ζ O , then for n 3 , we have ϕ ( ζ ) = ζ + ϕ 3 ζ 3 + .

4. Conclusions

From above, we proposed a new subclass of analytic normalized functions in the open unit disk. We presented a collection of results discussing the univalency and the stralikeness of the new class. Moreover, some recent works are indicated under our main results as consequences. For future work, one can make a development for the suggested class in view of other classes of analytic functions, such as the meromorphic, p-valent and harmonic classes. As an application, one can consider the suggested class operating with the class of special functions.

Author Contributions

Methodology, N.M.A. and M.O.; validation, N.M.A.; formal analysis, M.O.; writing M.O.; funding acquisition, N.M.A. All authors have read and agreed to the published version of the manuscript.

Funding

This research received no external funding.

Data Availability Statement

Data sharing is not applicable to this article as no data sets were generated or analyzed during the current study.

Conflicts of Interest

The authors declare no conflict of interest.

References

  1. Wang, Y.; Gu, Z.; Peng, W.; Shi, G.; Zhang, X.; Cui, Z.; Fu, P.; Qiao, X.; He, Y.; Liu, M.; et al. Silver Nanocrystal Array with Precise Control via Star-like Copolymer Nanoreactors. J. Phys. Chem. Lett. 2022, 13, 10823–10829. [Google Scholar] [CrossRef] [PubMed]
  2. Turpin, G.A.; Nelson, A.; Holt, S.A.; Giles, L.W.; Milogrodzka, I.; Horn, R.G.; Tabor, R.F.; van’t Hag, L. Investigating Adsorption of Cellulose Nanocrystals at Air–Liquid and Substrate–Liquid Interfaces after pH Manipulation. Adv. Mater. Interfaces 2023, 2202452. [Google Scholar] [CrossRef]
  3. Sajid, T.; Jamshed, W.; Ibrahim, R.W.; Eid, M.R.; Abd-Elmonem, A.; Arshad, M. Quadratic Regression Analysis for Nonlinear Heat Source/Sink and Mathematical Fourier Heat Law Influences on Reiner-Philippoff Hybrid Nanofluid Flow Applying Galerkin Finite Element Method. J. Magn. Magn. Mater. 2023, 568, 170383. [Google Scholar] [CrossRef]
  4. Bacova, P.; Gkolfi, E.; Harmandaris, V. Soft Character of Star-Like Polymer Melts: From Linear-Like Chains to Impenetrable Nanoparticles. Nano Lett. 2023, 23, 1608–1614. [Google Scholar]
  5. Ozaki, S. On the theory of multivalent functions. II. Sci. Rep. Tokyo Bunrika Daigaku Sect. A 1941, 4, 45–87. [Google Scholar]
  6. Umezawa, T. Analytic functions convex in one direction. J. Math. Soc. Jpn. 1952, 4, 194–202. [Google Scholar] [CrossRef]
  7. Sakaguchi, K. A property of convex functions and application to criteria for univalence. Bull. Natl. Univ. Educ. 1973, 22, 1–5. [Google Scholar]
  8. Luminita-Ioana, C.; Wanas, A.K. Applications of Laguerre Polynomials for Bazilevic and θ-Pseudo-Starlike Bi-Univalent Functions Associated with Sakaguchi-Type Functions. Symmetry 2023, 15, 406. [Google Scholar]
  9. Somya, M.; Ravichandran, V. On functions starlike with respect to n-ply symmetric, conjugate and symmetric conjugate points. arXiv 2022, arXiv:2201.01475. [Google Scholar]
  10. Hadid, S.; Ibrahim, R.W. On New Symmetric Schur Functions Associated with Integral and Integro-Differential Functional Expressions in a Complex Domain. Symmetry 2023, 15, 235. [Google Scholar] [CrossRef]
  11. Ibrahim, R.W. A new analytic solution of complex Langevin differential equations. Arab. J. Math. Sci. 2023, 29, 83–99. [Google Scholar] [CrossRef]
  12. Ibrahim, R.W.; Dumitru, B. Analytic studies of a class of Langevin differential equations dominated by a class of Julia fractal functions. Kragujev. J. Math. 2021, 48, 577–590. [Google Scholar]
  13. Hadid, S.B.; Ibrahim, R.W.; Momani, S. A new measure of quantum starlike functions connected with Julia functions. J. Funct. Spaces 2022, 2022, 4865785. [Google Scholar] [CrossRef]
  14. Mridula, M.; Kumar, S.S. Coefficient problems for certain Close-to-Convex Functions. Bull. Iran. Math. Soc. 2023, 49, 5. [Google Scholar]
  15. Ali, R.M.; Alarifi, Ṅ.M. The U-radius for classes of analytic functions. Bull. Malays. Math. Sci. Soc. 2015, 38, 1705–1721. [Google Scholar] [CrossRef]
  16. Duren, P.L. Univalent Functions; Grundlehren der Mathematischen Wissenschaften; Springer: New York, NY, USA, 1983; Volume 259. [Google Scholar]
  17. Friedman, B. Two theorems on schlicht functions. Duke Math. J. 1946, 13, 171–177. [Google Scholar] [CrossRef]
  18. Obradović, M.; Ponnusamy, S. On the class U. In Proceedings of the 21st Annual Conferance of the Jammu Mathematical Society, Srinagar, India, 19–20 October 2011; Volume 25, pp. 1–15. [Google Scholar]
  19. Jovanović, I.; Obradović, M. A note on certain classes of univalent functions. Filomat 1995, 9, 69–72. [Google Scholar]
  20. Miller, S.S.; Mocanu, P.T. Differential Subordinations; Marcel Dekker, Inc.: New York, NY, USA; Basel, Switzerland, 2000. [Google Scholar]
  21. Obradović, M.; Ponnusamy, Ṡ. New criteria and distortion theorems for univalent functions. Complex Var. Theory Appl. 2001, 44, 173–191. [Google Scholar] [CrossRef]
  22. Obradović, M.; Ponnusamy, S.; Singh, V.; Vasundhra, P. Univalency, starlikeness and convexity applied to certain classes of rational functions. Analysis 2002, 22, 225–242. [Google Scholar] [CrossRef]
  23. Shi, L.; Arif, M.; Bukhari, S.Z.H.; Raza, M.A. Some New Sufficient Conditions on p-Valency for Certain Analytic Functions. Axioms 2023, 12, 295. [Google Scholar] [CrossRef]
  24. Kumar, S.; Rath, B. The Sharp Bound of the Third Hankel Determinant for the Inverse of Bounded Turning Functions. Contemp. Math. 2023, 30–41. [Google Scholar] [CrossRef]
  25. Shi, L.; Arif, M.; Iqbal, J.; Ullah, K.; Ghufran, S.M. Sharp Bounds of Hankel Determinant on Logarithmic Coefficients for Functions Starlike with Exponential Function. Fractal Fract. 2022, 6, 645. [Google Scholar] [CrossRef]
  26. Mohsan, R.; Riaz, A.; Xin, Q.; Malik, S.N. Hankel Determinants and Coefficient Estimates for Starlike Functions Related to Symmetric Booth Lemniscate. Symmetry 2022, 14, 1366. [Google Scholar]
  27. Obradović, M.; Ponnusamy, Ṡ. Radius of univalence of certain class of analytic functions. Filomat 2013, 27, 1085–1090. [Google Scholar] [CrossRef]
  28. Obradović, M.; Ponnusamy, Ṡ. Criteria for univalent functions in the unit disk. Arch. Math. 2013, 100, 149–157. [Google Scholar] [CrossRef]
  29. Allu, V.; Pandey, A. The Zalcman conjecture for certain analytic and univalent functions. J. Math. Anal. Appl. 2020, 492, 124466. [Google Scholar]
  30. Li, L.; Ponnusamy, S.; Wirths, K.J. Relations of the class U (λ) to other families of functions. Bull. Malays. Math. Sci. Soc. 2022, 45, 955–972. [Google Scholar] [CrossRef]
  31. Patil, A.B.; Shaba, T.G. Sharp initial coefficient bounds and the Fekete–Szegö problem for some certain subclasses of analytic and bi-univalent functions. Ukr. Kyi Mat. Zhurnal 2023, 75, 198–206. [Google Scholar] [CrossRef]
  32. Ali, R.M.; Chung, Y.L.; Lee, S.K. On a Subclass of Analytic Functions Satisfying a Differential Inequality. Mediterr. J. Math. 2023, 20, 121. [Google Scholar] [CrossRef]
  33. Obradović, M.; Peng, Ż. Some new results for certain classes of univalent functions. Bull. Malays. Math. Sci. Soc. 2018, 41, 1623–1628. [Google Scholar] [CrossRef]
  34. Khan, S.; Altınkaya, Ş.; Xin, Q.; Tchier, F.; Malik, S.N.; Khan, N. Faber Polynomial Coefficient Estimates for Janowski Type bi-Close-to-Convex and bi-Quasi-Convex Functions. Symmetry 2023, 15, 604. [Google Scholar] [CrossRef]
  35. Ponnusamy, S.; Sahoo, Ṗ. Special classes of univalent functions with missing coefficients and integral transforms. Bull. Malays. Math. Sci. Soc. 2005, 28, 141–156. [Google Scholar]
  36. Sakar, F.M.; Ali Shah, S.G.; Hussain, S.; Rasheed, A.; Naeem, M. q-Meromorphic closed-to-convex functions related with Janowski function. Commun. Fac. Sci. Univ. Ank. Ser. Math. Stat. 2022, 71, 25–38. [Google Scholar] [CrossRef]
  37. Sakar, F.M.; Naeem, M.; Khan, S.; Hussain, S. Hankel determinant for class of analytic functions involving Q-derivative operator. J. Adv. Math. Stud. 2021, 14, 265–278. [Google Scholar]
Figure 1. Plot of ϕ ( ζ ) = ζ / ( 1 ζ ) and its bounded turning behavior, respectively.
Figure 1. Plot of ϕ ( ζ ) = ζ / ( 1 ζ ) and its bounded turning behavior, respectively.
Symmetry 15 01014 g001
Disclaimer/Publisher’s Note: The statements, opinions and data contained in all publications are solely those of the individual author(s) and contributor(s) and not of MDPI and/or the editor(s). MDPI and/or the editor(s) disclaim responsibility for any injury to people or property resulting from any ideas, methods, instructions or products referred to in the content.

Share and Cite

MDPI and ACS Style

Alarifi, N.M.; Obradović, M. Univalence and Starlikeness of Certain Classes of Analytic Functions. Symmetry 2023, 15, 1014. https://doi.org/10.3390/sym15051014

AMA Style

Alarifi NM, Obradović M. Univalence and Starlikeness of Certain Classes of Analytic Functions. Symmetry. 2023; 15(5):1014. https://doi.org/10.3390/sym15051014

Chicago/Turabian Style

Alarifi, Najla M., and M. Obradović. 2023. "Univalence and Starlikeness of Certain Classes of Analytic Functions" Symmetry 15, no. 5: 1014. https://doi.org/10.3390/sym15051014

Note that from the first issue of 2016, this journal uses article numbers instead of page numbers. See further details here.

Article Metrics

Back to TopTop