Abstract
In this paper, two new classes of q-starlike functions in an open unit disc are defined and studied by using the q-fractional derivative. The class , , generalizes the class of q-starlike functions and the class , , comprises the q-starlike univalent functions with negative coefficients. Some basic properties and the behavior of the functions in these classes are examined. The order of starlikeness in the class of convex function is investigated. It provides some interesting connections of newly defined classes with known classes. The mapping property of these classes under the family of q-Bernardi integral operator and its radius of univalence are studied. Additionally, certain coefficient inequalities, the radius of q-convexity, growth and distortion theorem, the covering theorem and some applications of fractional q-calculus for these new classes are investigated, and some interesting special cases are also included.
Keywords:
analytic functions; starlike functions; q-fractional differential operator; fractional derivative; q-starlike functions; q-Bernardi operator MSC:
30C45; 30C50
1. Introduction
Quantum calculus is basically usual calculus without the notion of limits. It has wide applications in mathematics and physics. The q-derivative and q-integral are the main tools introduced by Jackson [1,2] in a systematic way. The linear q-difference equation, and q-differential equations, are studied in [3,4]. Mansour [5] investigated linear sequential q-differential equation of fractional order. Using the q-derivative, Ismail [6] introduced the class of q-starlike functions. In the recent past, the theory of q-calculus operators has been applied in general fractional calculus. Al-Salam [7] and Agarwal [8] introduced several types of fractional q-integral operators and fractional q-derivatives. Rajkovi’c [9] investigated fractional integral and derivatives in q-calculus. Additionally, q-integral operators for certain analytic functions by using the concept and theory of fractional q-calculus that was studied by Selvakumaran et al. [10]. Recently, researchers proposed q-version of well known operators like Baskakov Durrmeyer operator, Picard integral operator, Bernardi integral operator and the Gauss–Weierstrass integral operator, see [11,12,13,14,15]. Furthermore, Purohit and Raina [16] applied q-operators on subclasses of analytic functions. Ismail [6] introduced the well known class of q-starlike functions related to q-derivative operator [16,17]. Wingsaijai and Sukantmala [18] presented the class of q-starlike functions of order , , Certain Coefficient Estimate Problems for Three-Leaf-Type Starlike Functions. Sahoo and Sharma [17] defined and studied analogue of a close-to-convex function.
The starlikeness of normalized bessel functions with symmetric points is studied in [19]. Recently, certain generalized classes of q-starlike functions have been investigated, see [20,21]. Zainab et al. [22] defined a new class of q-starlike functions by using q-Ruscheweyh differential operator. The recent contributions on fractional derivatives by several researchers are also worth reading, see [23,24,25]. Sokół [26] introduced a one-parameter family of functions , as shown in (5). Using this family of functions, he defined a classes of starlike functions, and certain properties of these functions were investigated. However, has not been studied under the q-analogue of analytic and univalent functions of negative order, which has vital applications in different zones of mathematics. This was the main motivation behind Definitions 1 and 3 and their related results, and to keep in mind recent developments on starlike functions and their associated functions, we have categorized our main results into two sections. In the first section, we have investigated some interesting properties for our new class , of q-starlike functions of order , , which is introduced in Definition 1. We primarily focus on q-integral representation of functions belonging to this class, and its related results. Further, we have investigated distortion bounds and order of starlikeness in class of convex functions. In the second section, we have defined the class of q-starlike functions of order ( ) with negative coefficients. It is investigated that functions belonging to this class are preserved under q-Bernardi integral operator and its radius of univalence is also determined. Several other properties such as coefficient inequities, radius of q-convexity, growth and distortion theorem, covering result and some applications of fractional q-calculus for the said class are presented. It is noted that obtained results are the advancement of several known results, proved by researchers in their research articles.
Let A consist of the analytic functions of the form
Let be the class of univalent functions in . The classes of starlike functions of order and of convex functions of order , which are subclasses of S are defined as:
When , we have the well-known class of starlike functions and the class C of convex functions, see [27]. Let , . Then, we say that is subordinate to , written as , if there exists a function w, analytic in E with and , , such that If , it is known that the above subordination is equivalent to and , see [27].
Let T denote the subclass of S consisting of the analytic and univalent functions, whose functions can be expressed as
Silverman [28] introduced and studied the classes and of starlike functions of order and convex functions of order , in the open unit disc . He defined these classes as follows:
When , the above classes reduce to the classes and K, of starlike and convex functions of negative coefficients, respectively, see [28].
Our work is related to a one-parameter family of functions defined and studied by Sokół [26]. We recall the properties of these functions, which we shall need to derive our results.
Remark 1.
Let
Then, the following assertions are true.
- 1.
- is univalent in E.
- 2.
- 3.
- When , is convex univalent function in E.
Now, we include some basic definitions and concepts of q-calculus, which are used in this work.
The q-derivative of a function is defined by
and , where , see [2]. For a function , the q-derivative is
where
We note that as , , here is ordinary derivative and as . From (4), one can deduce that
Jackson [1] introduced the q-integral of a function f, which is given by
provided that series converges.
In [18], Wongsaijai and Sukantamala introduce the class of q-starlike functions of order as follows:
The corresponding class of q-convex functions is defined as
By seting in above definitions, we get of q-convex functions and of q-starlike functions introduced in [6].
Then, we define a new class , which is the refinement of the above known classes of starlike functions. Results related to this class will be derived in Section 2.
Definition 1.
A function from the class A is said to be in the class if and only if it satisfies the condition
where is given by (5).
From the Remark 1, we have
when .
Our aim is to investigate geometric properties of class of q-starlike functions of order . It deals with several ideas and techniques used in geometric function theory. The order of starlikeness in the class of convex functions of negative order and distortion bounds is also formulated. It provides an interesting connection of our above-defined class with well known classes in the form of following special cases.
Special Cases
- 1.
- When , we have
- 2.
- For , we obtain
- 3.
- Let , and taking , we get the class of starlike functions, which is univalent in E, see [27].
- 4.
- If , then f belongs to the class of q-starlike functions, which is defined and studied in [6].
- 5.
- For , we have the known class of q-starlike functions of order , see [27].
- 6.
- When , then f belongs to the class of starlike function with order .
Now we define another class , a subclass of . This class will be used in derivation of Theorems 1 and 8.
Definition 2.
For , , the class is defined as follows.
We note that, for , then the function maps the unit disc E onto half plane and onto the disc with center and radius , for .
Next, we define the class of q-starlike functions of order with negative coefficients. Results regarding this class are presented in Section 3.
Definition 3.
A function from the class T is said to be in the class if and only if it satisfies the condition
Special Cases
- 1.
- If , we havewhich contains q-starlike functions with negative coefficients, and taking , we obtain the known class introduced in [28].
- 2.
- For , we haveof q-starlike functions of order with negative coefficients, and taking , we obtain the known class K of convex functions defined and studied in [28].
- 3.
- When , we obtainof starlike function of order with negative coefficients.
Next, we define the corresponding class of q-convex functions of order and having negative coefficients. An application of this class will be shown in investigating the radius problem as given in Theorem 10.
Definition 4.
A function from the class T is said to be in the class if and only if it satisfies the condition
We require following lemma to obtain our main results.
Lemma 1
(q-Jack’s Lemma, [29]). Let be analytic in E with . Then, if attains its maximum value on the circle at a point , then we have
real number.
2. The Class
In this section, we obtain some results related to newly defined class of q-starlike functions of order . For the following results, we consider , , , unless otherwise stated. To prove our main results, we first prove the following lemma.
Lemma 2.
Let h be analytic in E with . A function G is in the class
if and only if there exists an analytic function , , such that
Proof.
Consider
where is analytic and in E. Using q-integral properties, we get
Using the formulation , and the fundamental theorem of q-calculus, see [30], we get
which implies that
it follows that , and this implies that in E. This completes the proof. □
By taking in Lemma 2, we obtain the known result proved by Sokół [26].
Then, by using the class given by (15), we derive the following theorem for the function , .
Theorem 1.
Let , . If , then there exists a function and the function , such that
(We note that, if ; then,
Proof.
Let . Then, by Lemma 2, there exists an analytic function with and , , such that
and from (5), we have
which implies that
It follows that
This implies that
Using the Lemma 2, we have
which shows that the functions and satisfy and , and this completes the proof. □
Theorem 2.
Let , . If there exists a function and , such that
and
for analytic function , and , , then the function
Proof.
From (23) and (24), we find that and are generated by (19) wih the same function w, so by using Theorem 1 and Lemma 2, we have
Hence, we have
which is the required result. □
Next, we obtain distortion result for our class , by using Theorems 1 and 2.
Theorem 3.
If , , and , , then
Proof.
Let . Then, by Theorem 1, there exist and , such that (25) holds.
Let . Then, we have
which implies that
Using q-differential properties and partial q-derivatives, we get
The q-integration gives us
Raising (26) to power , we get
Now, we suppose that , so we can write
It follows that
as the linear transformation maps onto disc of center and radius . Additionally, we know that
so, we have
The q-Integration on both sides gives us
Next, we will obtain the order of starlikeness in the class of convex functions.
Theorem 4.
Let , and let , for ,
Then,
Proof.
On contrary, we assume , such that , and , ; thus, we have
Re-substituting , and since , so we have
where which is contraction to our given hypothesis. Thus, the required result follows. □
We note that by substituting various values to the parameters involved in above result, we get known and new results, as shown in the following corollaries.
Corollary 1.
Let , and . Then, if
then
By further taking , we obtain the well known result that a convex function of order zero is starlike of order one-half, see [27].
Corollary 2.
Let , and . Then,
implies that
Corollary 3.
Let and . Then, if
then
The following theorem shows the coefficients inequality for the functions of the class
Theorem 5.
Proof.
It is sufficient to prove that the values for lie in a circle centered at 1 and radius . For this, consider
However, (35) is true by hypothesis. Thus, we have , and this gives us the required result. □
Taking and in Theorem 5, we get the following known result.
Corollary 4
([31]). Let , . Then, if
then .
Taking , and in Theorem 5, we obtain a result proved by Schild [32], as shown in the following corollary.
Corollary 5
([32]). Let Then, if
then .
Set in Theorem 5, this gives us the following result.
Corollary 6.
Let Then, if
then .
3. The Class
In this section, we shall study the properties of the class shown in Definition 3. For the following results, we have , unless otherwise stated.
3.1. Coefficient Inequalities
Coefficient inequalities for functions belong to the class are derived in following theorem.
Theorem 6.
Let f be given by (4). Then, , if and only if
Proof.
In view of Theorem 5, it is sufficient to prove the only if part. Let , that is,
Choose values of z on real axis so that is real. Upon clearing the denominator in (40), and letting through real values, we have
By (8), we have
and this completes the proof. □
Corollary 7.
Let . Then, if , then
This result is sharp for the extremal function of the form
3.2. Distortion Theorems
The growth and distortion theorems for the functions in the class , for .
Theorem 7.
Let . If , then
Equality holds for the extremal function , given as
Proof.
From Theorem 6, we have
That is,
Theorem 8.
Proof.
Consider
From Theorem 6, we have
Similarly, we have
This completes the proof. □
Setting and in Theorems 7 and 8, we get the results, derived by Silverman [28].
3.3. Covering Results
Following is the covering result deduced by letting in Theorem 7.
Theorem 9.
Let Let , and let . Then, contains an open unit disc of radius
Equality holds for the function given by (44).
3.4. Radius of q-Convexity for
Now, we investigate the radius of q-convexity for functions in class .
Theorem 10.
Let and let . Then, f is q-convex in the disk
This result is sharp. Extremal function is given by (44).
Proof.
We are required to show that for , we have
The left side of expression given in (52) is bounded above by 1 if
or
which will be true, if by Theorem 6,
It follows that
Set , we have
which is the required result. □
Taking and in Theorem 10, we obtain the known result, see [28].
3.5. Integral Operators
In [15], q-Bernardi operator is defined as:
Let , and let , . Then,
We note that is well defined. Next, we prove that the class is closed under q-Bernardi operator given by (54) for , and f is defined by (4), and we also discuss the converse case by investigating the radius of univalence.
Theorem 11.
Proof.
Consider
as . Therefore, an application of Theorem 6 leads us to the fact that , which is the required result. □
Next, we will investigate the radius problem for the function given in (54). For this purpose, we prove the following lemma.
Lemma 3.
(q-Noshiro–Warchowsky theorem) Let . If for all z belongs to a convex domain D and some real α, , then f is said to be a univalent function in E.
Proof.
Since , so
and also we have ; therefore, by Fundamental Theorem of q-Calculus, see [30], we have . Thus, is univalent in D. □
Taking in above lemma, we get the well known Noshiro–Warchowsky theorem, see [27].
Theorem 12.
Let c be real number such that . If ; then, f is defined by (4) is univalent in , where
This result is sharp.
3.6. Extreme Points for
To investigate the extreme points of , we have the following theorem.
Theorem 13.
Let , and
Then, if and only if it has the form
where and .
Proof.
Let
Then, from Theorem 6, we have
Thus . Conversely, let ; from Corollary 7, we have
We may set
and
It follows that
and this completes the proof. □
Corollary 8.
The extreme points of are functions given by (62),
We take and , and this leads us the result derived in [28].
Remark 2.
We note that our Theorems 6 and 7 can be derived alternatively by analysis of extreme points shown in above theorem.
3.7. Application of the Fractional Calculus
In recent past years, the theory of q-calculus operators has been applied in the areas of ordinary fractional calculus, see [3,5,33,34]. Using the concepts of q-theory, Al-Salam [7] and Agarwal [8] introduced fractional q-integral operator and fractional q-derivatives operator as follows.
Definition 5.
The fractional q-integral operator of a function of order , is given by
where is analytic function in simply connected region of z-plane containing the origin. Here, the term is q-binomial function defined by
Definition 6.
The fractional q-derivative operator of function of order , is defined by
where is suitably contained and the multiplicity of is removed as in Definition 5.
Definition 7.
Fractional q-derivative of order is defined by
where and
Next, we use the fractional q-derivative operator and fractional q-integral operator to prove the following results for the class .
Theorem 14.
Let , , and the function f defined by (4) be in the class . Then, we have
and
Equality holds for the function
Proof.
From (69), we have
where
is decreasing in n, so by using the properties of q-gamma function, we have
and from Theorem 6, we have
Additionally, we have
Equality holds for the function
This completes the proof. □
Theorem 15.
Let , , and the function f defined by (4) be in the class . Then, we have
and
Equality holds for the function
Proof.
From (69), we have
where
is decreasing in n, so we have
and an application of Theorem 6, we have
Additionally, we have
Equality holds for the function
This completes the proof. □
Corollary 9.
Proof.
By Definition 5 and Theorem 15, if we take , this gives us and the result is true. Additionally, from Definition 6 and Theorem 14, for , we have , and hence we get the required result. □
4. Conclusions
We introduced and studied two classes of starlike functions defined by q-fractional derivative; one contains negative coefficients and one is of negative order. Both these classes were discussed in detail, and certain geometrical properties were investigated that generalized the already known results. We note that results proved in this article are the q-extension and advancements of several results investigated in [26,28,31,32].
Author Contributions
Conceptualization, S.R. and Q.X.; methodology, S.R. and Q.X.; software, S.N.M.; validation, S.N.M. and A.R.; formal analysis, S.N.M. and A.R.; investigation, S.R.; resources, Q.X. and U.A.N.; data curation, S.R.; writing—original draft preparation, S.R.; writing—review and editing, S.N.M.; visualization, U.A.N.; supervision, S.N.M.; project administration, Q.X.; funding acquisition, S.R. and S.N.M. All authors have read and agreed to the published version of the manuscript.
Funding
This research received no external funding.
Institutional Review Board Statement
Not applicable.
Informed Consent Statement
Not applicable.
Data Availability Statement
Not applicable.
Acknowledgments
The authors acknowledge the heads of their institutes for their support and for providing the research facilities.
Conflicts of Interest
The authors declare no conflict of interest.
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