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Article

Applications of Symmetric Conic Domains to a Subclass of q-Starlike Functions

1
Department of Mathematics, Riphah International University, Islamabad 44000, Pakistan
2
Department of Mathematics, Abbottabad University of Science and Technology, Abbottabad 22010, Pakistan
3
Department of Mathematics, King Abdulaziz University, P.O. Box 80203, Jeddah 21589, Saudi Arabia
4
Department of Economics, Faculty of Economics Administrative and Social Sciences, Hasan Kalyoncu University, Gaziantep TR-27410, Turkey
5
School of Mathematical Sciences and Shanghai Key Laboratory of PMMP, East China Normal University, 500 Dongchuan Road, Shanghai 200241, China
*
Author to whom correspondence should be addressed.
Submission received: 22 March 2022 / Revised: 7 April 2022 / Accepted: 11 April 2022 / Published: 12 April 2022
(This article belongs to the Special Issue Symmetry in Pure Mathematics and Real and Complex Analysis)

Abstract

:
In this paper, the theory of symmetric q-calculus and conic regions are used to define a new subclass of q-starlike functions involving a certain conic domain. By means of this newly defined domain, a new subclass of normalized analytic functions in the open unit disk E is given. Certain properties of this subclass, such as its structural formula, necessary and sufficient conditions, coefficient estimates, Fekete–Szegö problem, distortion inequalities, closure theorem and subordination results, are investigated. Some new and known consequences of our main results as corollaries are also highlighted.

1. Introduction and Definitions

Let A denote the class of all analytic functions f which are analytic in the open unit disk
E = { z : z C and z < 1 }
and series expansion is
f ( z ) = z + n = 2 a n z n .
The usage of normalize functions in geometric function theory is significant. They are used to map everything inside a unit circle, where everything is convergent. Using this concept, many different subclasses of analytic functions have been defined and studied.
Furthermore, let S A represents the set of all univalent in E (see [1,2]). The classes of uniformly convex UCV and uniformly starlike ( UST ) functions were introduced by Goodman [3] and are defined analytically as:
f UCV f A and z f ( z ) f ( z ) < 1 + z f ( z ) f ( z ) z E
and
f UST f A and z f ( z ) f ( z ) 1 < z f ( z ) f ( z ) , z E .
The classes of k-uniformly convex k - UCV and k-uniformly starlike k - UST functions were introduced by Kanas and Wisniowska in [4] and are defined analytically as:
f ( z ) k - UST f ( z ) A and 1 > k z f ( z ) f ( z ) 1 z f ( z ) f ( z ) , z E ,
and
f ( z ) k - UCV f ( z ) A and 1 > k z f ( z ) f ( z ) 1 + z f ( z ) f ( z ) , z E .
Note that
f ( z ) k - UCV z f ( z ) k - ST .
The above-defined function classes were studied and investigated by a number of well-known mathematicians; see for details [1,2,3,4,5,6].
Two analytic functions f and g are subordinate to each other, (written as f ( z ) g ( z ) ), if there exists a Schwarz function s ( z ) , which is analytic in E with
s ( 0 ) = 0 and | s ( z ) | < 1
such that
f ( z ) = g ( s ( z ) ) .
Additionally, if g ( z ) S in E, then we have (see [1,2])
f ( z ) g ( z ) f ( 0 ) = g ( 0 ) and f ( E ) g ( E ) .
The convolution of two analytic functions
f ( z ) = n = 0 a n z n and g ( z ) = n = 0 b n z n , ( z E )
is defined as:
f g ( z ) = n = 0 a n b n z n .
Let P represent the set of all of Carathéodory functions and every analytic function p P , having series of the form
p ( z ) = 1 + n = 1 c n z n
and satisfying the condition
p ( z ) > 0 , z E .
In terms of these analytic functions, many different subclasses of starlike and convex functions have been defined already.
We have discussed above that Kanas and Wisniowska [4] introduced the class of k-uniformly convex functions k - UCV and the corresponding class of k-starlike functions k - ST and then defined these classes subject to the conic domain Ω k , ( k 0 ) as follows:
Ω k = u + i v : u > k u 1 2 + v 2 ,
or
Ω k = w : w > k w 1 .
For k = 0 , then (2) becomes the right half plane; for 0 < k < 1 , it becomes a hyperbola, for k = 1 it becomes a parabola and for k > 1 , it becomes an ellipse. The generalization of theses discussed by Shams et al. in [7] is subject to the conic domain Ω k , γ ( k 0 ) , γ C \ { 0 } , which is
Ω k , γ = u + i v : u > k u 1 2 + v 2 + γ ,
or
Ω k , γ = w : w > k w 1 + γ .
For this conic domain, the function p k , γ ˜ ( z ) plays the role of the extremal function for the conic domain Ω k , γ .
p k , γ ˜ ( z ) = 1 + z 1 z for k = 0 , 1 + 2 γ π 2 log 1 + z 1 z 2 for k = 1 , 1 + 2 γ 1 k 2 H 1 ( k , z ) for 0 < k < 1 , 1 + γ k 2 1 H 1 ( k , z ) + γ 1 k 2 for k > 1 ,
where
H 1 ( k , z ) = sinh 2 2 π arccos k arctan h z
H 2 ( k , z ) = sin π 2 K ( i ) 0 u ( z ) t 1 1 x 2 1 ( i x ) 2 d x
and i ( 0 , 1 ) , k = cosh π K ( i ) 4 K ( i ) , K ( i ) is the first kind of Legendre’s complete elliptic integral. For details (see [4]). Indeed, from (3), we have
p k , α ˜ ( z ) = 1 + Q 1 z + Q 2 z 2 + . . . ,
where
Q 1 = 2 γ 2 π arccos k 2 1 k 2 for 0 k < 1 , 8 γ π 2 for k = 1 , H 3 ( k , z ) for k > 1 ,
Q 2 = 2 π arccos k 2 + 2 3 Q 1 for 0 k < 1 , 2 3 Q 1 for k = 1 , H 4 ( k , z ) Q 1 for k > 1 ,
and
H 3 ( k , z ) = π 2 γ 4 1 + t t K 2 ( t ) k 2 1 , H 4 ( k , z ) = 4 K 2 ( t ) t 2 + 6 t + 1 π 2 24 K 2 t 1 + t t .
In the twentieth century the researchers have developed a great interest in the study of theory of q-calculus and its numerous applications in the fields of mathematics and physics. In defining the q-analogous of the derivative and integral operator and providing few of their applications, Jackson [8] was one of the pioneer researchers. It has several applications in number theory, combinatorics, orthogonal polynomials, fundamental hyper-geometric functions, and other fields of mathematics, including quantum mechanics, mechanics and relativity theory. Furthermore, quantum calculus has been proven to be a branch of the more comprehensive mathematical area of time scale calculus. For both discrete and continuous domains, time scales provide a coherent framework for studying dynamic equations. Many researchers provided useful applications for q-analysis in domains of mathematics; see [9,10,11,12,13,14,15,16,17,18]. Currently, operators of basic (or q-) calculus and fractional q-calculus and their applications have been elaborated by Srivastava in [19]. Considering the importance of q-operator calculus theory, researchers have intensively explored their applications in various fields; see [20,21,22,23,24,25].
In many areas of mathematics, the symmetric properties of functions play an important role in problem solving. Symmetry’s importance has been demonstrated in a variety of fields, including biology, chemistry, and psychology. Recently, in [26], Zhang et al. studied the application of a q-symmetric difference operator in harmonic univalent functions. Additionally, Khan et al. [27] defined the symmetric conic domain by using symmetric q-calculus operator theory and investigated q-starlike functions in this domain. Very recently, Khan et al. [28] defined and explored a new subclass of analytic and bi-univalent function involving certain q-Chebyshev polynomials by means of a symmetric q-operator. The symmetric q-calculus finds its applications in different fields, especially in quantum mechanics; see for example [29,30].
Here we present a few basic definitions, as well as a concept of q-calculus and symmetric q-calculus which will help us in further studies.
Definition 1
([31]). The q-number [ t ] q for q ( 0 , 1 ) is defined as:
[ t ] q = 1 q t 1 q , ( t C ) .
For ( t = n N ) , then
[ t ] q = k = 0 n 1 q k
and the q-gamma function is defined by:
Γ q ( t + 1 ) Γ q ( t ) = [ t ] q
and
Γ q ( 1 ) = 1 .
Definition 2
([27]). For n N , the symmetric q-number is defined as:
[ n ] ˜ q = q n q n q 1 q , [ 0 ] ˜ q = 0 .
Remark 1.
The symmetric q-number can not reduce to a q-number.
Definition 3
([27]). The q-factorial [ n ] q ! for q ( 0 , 1 ) is defined as:
[ n ] q ! = k = 1 n [ k ] q , ( n N )
and
[ 0 ] q ! = 1 .
Definition 4
([27]). For any n Z + 0 , the symmetric q-number shift factorial is defined as:
[ n ] ˜ q ! = [ n ] ˜ q [ n 1 ] ˜ q [ n 2 ] ˜ q . . . [ 2 ] ˜ q [ 1 ] ˜ q , n 1 1 n = 0 .
Note that
lim q 1 [ n ] ˜ q ! = n ! .
Definition 5
([32]). Let f A ; then, the symmetric q-derivative operator is defined by:
D ˜ q f ( z ) = 1 z f ( q z ) f ( q 1 z ) q q 1 , z E .
We can write (8) as:
D ˜ q f ( z ) = 1 + n = 1 [ n ] ˜ q a n z n 1 .
Note that
D ˜ q z n = [ n ] ˜ q z n 1 , D ˜ q n = 1 a n z n = n = 1 [ n ] ˜ q a n z n 1 ,
and
lim q 1 D ˜ q f ( z ) = f ( z ) .
Definition 6
([27]). Let f A and 0 < q < 1 ; then f S q ˜ if
f ( 0 ) = f ( 0 ) = 1
and
z D ˜ q f ( z ) f ( z ) 1 1 q q 1 1 1 q q 1 .
Using the definition of subordination, we can write the condition in (9) as:
w D ˜ q g ( z ) g ( z ) 1 + z 1 q q 1 z .
Recently, several classes of analytic and univalent functions in different types of domains have investigated in [21,22,27,33,34,35,36,37,38,39,40,41,42,43]. For example, let p ( z ) be an analytic in E and p ( 0 ) = 1 . Then:
(i)
The image domain of E under p ( z ) lies in right half plane if p ( z ) 1 + z 1 z (see [3]);
(ii)
For 1 B < A 1 , the image of E under p ( z ) lies inside a circle centered on real axis if p ( z ) 1 + A z 1 + B z (see [44]);
(iii)
For 0 α < 1 , in [4,34], Kanas showed that the image of E under p ( z ) lies inside the conic domain Ω k and Ω k , α if
p ( z ) p k , α ( z ) ;
(iv)
For γ C \ { 0 } , in [7], Shams et al. showed that the image of U under p ( z ) lies inside the conic domain Ω k , γ if
p ( z ) p k , γ ( z ) .
By taking motivation from the above-cited works, we define the following domain:
Definition 7.
Let k [ 0 , ) , q 0 , 1 and γ C \ { 0 } . A function p ( z ) is said to be in the class k- P ˜ q , q 1 , γ ( z ) if and only if
p ( z ) p k , q , q 1 , γ ˜ ( z )
where
p k , q , q 1 , γ ˜ = 2 q 1 p k , γ ˜ ( z ) q 1 + q + q 1 q p k , γ ˜ ( z )
and p k , γ ˜ ( z ) is given by (3). Geometrically, the function p ( z ) k - P ˜ q , q 1 , γ ( z ) takes on all values from the domain Ω k , q , q 1 , γ ˜ which is defined as:
Ω k , q , q 1 , γ ˜ = γ Ω k , q , q 1 ˜ + ( 1 γ ) ,
where
Ω k , q , q 1 ˜ = w : q 1 + q w ( z ) q q 1 w ( z ) + 2 q 1 > k q 1 + q w ( z ) q q 1 w ( z ) + 2 q 1 1 .
Remark 2.
(i) First of all, we see that
lim q 1 Ω k , q , q 1 , γ ˜ = Ω k , γ ( γ C \ { 0 } )
where Ω k , γ is the conic domain considered by Shams et al. [7]. Secondly, we have
lim q 1 Ω k , q , q 1 , 1 ˜ = Ω k ,
where Ω k is the conic domain considered by Kanas and Wisniowska [34]. Thirdly, we have
lim q 1 k - P q , q 1 , 1 = P ( p k ) ,
where P ( p k ) is the well-known class introduced by Kanas and Wisniowska [34]. Lastly, we have
lim q 1 0 - P q , q 1 , 1 = P ,
where P is the well-known class of analytic functions with a positive real part.
Using the above-defined domain, we now define the following subclass of certain analytic functions:
Definition 8.
An analytic function f k- UST ( q , q 1 , γ ) if it satisfies the condition
1 + 1 γ J ( q , q 1 , f ( z ) ) 1 > k 1 γ J ( q , q 1 , f ( z ) ) 1 ,
or equivalently
J ( q , q 1 , f ( z ) ) k P ˜ q , q 1 , γ ,
where
J ( q , q 1 , f ( z ) ) = q 1 + q z D ˜ q f ( z ) f ( z ) q q 1 z D ˜ q f ( z ) f ( z ) + 2 q 1 .
Remark 3.
First of all, we have (see [34])
lim q 1 k - UST ( q , q 1 , γ ) = S k , γ .
Secondly, it could be seen that (see [4])
lim q 1 k - UST ( q , q 1 , 1 ) = k - UCV .
Geometrically, the function f A is in the class k- UST ( q , q 1 , γ ) , if and only if the function J ( q , q 1 , f ( z ) ) takes all values in the conic domain Ω k , q , q 1 , γ ˜ given by (12). Taking this geometrical interpretation into consideration, one can rephrase the above definition as:
Definition 9.
An analytic function f k- UST ( q , q 1 , γ ) if and only if
J ( q , q 1 , f ( z ) ) p k , q , q 1 , γ ˜ ( z ) ,
where p k , q , q 1 , γ ˜ ( z ) is defined by (11).
We also fixed k- UST ( q , q 1 , γ ) = k - UST ( q , q 1 , γ ) T , where T is the subclass of k- UST ( q , q 1 , γ ) consisting of functions of the form
f ( z ) = z n = 2 a n z n , a n 0 , n 2 .
Our further investigation is organized as follows. In Section 2, we give some supporting results in form of Lemmas, which will help in order to obtain our new results in Section 3. In Section 3, we obtain our main results and also give some of their special cases in the form of Corollaries and Remarks. In Section 4, we conclude our present investigation and also give some future direction to the interested readers toward the prospect that this kind of result will be obtained for other new subclasses of analytic functions.

2. A Set of Lemmas

We need the following lemmas in order to prove our main results.
Lemma 1
(See [45]). Let p ( z ) = 1 + n = 1 p n z n F ( z ) = 1 + n = 1 d n z n . If F ( z ) is convex univalent in E , then
p n d 1 , n 1 .
Lemma 2.
Let k [ 0 , ) be fixed and
p k , q , q 1 , γ ˜ ( z ) = 2 q 1 p k , γ ˜ ( z ) q 1 + q + q 1 q p k , γ ˜ ( z ) .
Then
p k , q , q 1 , γ ˜ ( z ) = 1 + 2 q 1 q 1 + q Q 1 z + 2 q 1 q 1 + q Q 2 2 ( q 1 q ) q 1 + q Q 1 2 z 2 + ,
where Q 1 , and Q 2 is given by (5) and (6)
Proof. 
From (11), we have
p k , q , q 1 , γ ˜ ( z ) = 2 q 1 p k , γ ˜ ( z ) q 1 + q + q 1 q p k , γ ˜ ( z ) = 2 q 1 q 1 + q p k , γ ˜ ( z ) 2 q 1 ( q 1 q ) q 1 + q 2 p k , γ ˜ ( z ) 2 + 2 q 1 ( q 1 q ) 2 q 1 + q 3 p k , γ ˜ ( z ) 3 2 q 1 ( q 1 q ) 3 q 1 + q 4 p k , γ ˜ ( z ) 4 + .
By using (4) in (18), we have
p k , q , q 1 , γ ˜ ( z ) = n = 1 2 q 1 1 n 1 ( q 1 q ) n 1 q 1 + q n + n = 1 2 q 1 n 1 n 1 ( q 1 q ) n 1 q 1 + q n Q 1 z + n = 1 2 q 1 n 1 n 1 ( q 1 q ) n 1 q 1 + q n Q 2 n = 1 2 q 1 ( 2 n 1 ) 1 n 1 ( q 1 q ) n q 1 + q n + 1 Q 1 2 z 2 + .
The series n = 1 2 q 1 1 n 1 ( q 1 q ) n 1 q 1 + q n , n = 1 2 q 1 n 1 n 1 ( q 1 q ) n 1 q 1 + q n , and
n = 1 2 q 1 ( 2 n 1 ) 1 n 1 ( q 1 q ) n q 1 + q n + 1 are convergent and convergent to 1 , 2 q 1 q 1 + q , and 2 q 1 ( q 1 q ) q 1 + q respectively.
Therefore, (19) becomes
p k , q , q 1 , γ ˜ ( z ) = 1 + 2 q 1 q 1 + q Q 1 z + 2 q 1 q 1 + q Q 2 2 q 1 ( q 1 q ) q 1 + q Q 1 2 z 2 + .
This complete the proof of Lemma 2. □
Remark 4.
For q 1 , Lemma 2 reduces to the lemma introduced by Sim et al. [46].
Lemma 3.
Let p ( z ) = 1 + n = 1 p n z n k - P ˜ q , q 1 , γ ; then
p n 2 q 1 q 1 + q Q 1 , n 1 .
Proof. 
By definition (7), a function p ( z ) k - P ˜ q , q 1 , γ ( z ) if and only if
p ( z ) p k , q , q 1 , α ˜ ( z ) ,
where k [ 0 , ) , and p k , q , q 1 , γ ˜ ( z ) is given by (11).
By using (20) in (21), we have
p ( z ) 1 + 2 q 1 q 1 + q Q 1 z + 2 q 1 q 1 + q Q 2 2 q 1 ( q 1 q ) q 1 + q Q 1 2 z 2 + .
Now by using Lemma 1 on (22), we have
p n 2 q 1 q 1 + q Q 1 .
Hence, the proof of Lemma 3 is complete. □
Remark 5.
For q 1 , then Lemma 3 reduces to the lemma introduced by Noor et al. [47].
Lemma 4
([48]). Let h ( z ) = 1 + n = 1 c n z n and h ( z ) be analytic in E and satisfy { h ( z ) } > 0 for z in E. Then,
c 2 v c 1 2 2 max 1 , 2 v 1 , v C .

3. Main Results

We now state and prove our main results. The first theorem of this section gives necessary conditions for an analytic function f of the form (1) to belong to the newly defined class k- UST ( q , q 1 , γ ) .
Theorem 1.
If an analytic function f is of the form (1), and it satisfies
n = 2 2 q 1 ( k + 1 ) [ n ] ˜ q 1 + γ q q 1 [ n ] ˜ q + 2 q 1 a n q + q 1 γ ,
then f k - UST ( q , q 1 , γ ) .
Proof. 
Suppose that 23 holds; then, it is sufficient to show that
k γ J ( q , q 1 , f ( z ) ) 1 1 γ J ( q , q 1 , f ( z ) ) ) 1 1 .
Using (15), we have
k γ q 1 + q z D ˜ q f ( z ) f ( z ) q q 1 z D ˜ q f ( z ) f ( z ) + 2 q 1 1 1 γ q 1 + q z D ˜ q f ( z ) f ( z ) q q 1 z D ˜ q f ( z ) f ( z ) + 2 q 1 1 k γ q 1 + q z D ˜ q f ( z ) f ( z ) q q 1 z D ˜ q f ( z ) f ( z ) + 2 q 1 1 + 1 γ q 1 + q z D ˜ q f ( z ) f ( z ) q q 1 z D ˜ q f ( z ) f ( z ) + 2 q 1 1 , ( k + 1 ) γ q 1 + q z D ˜ q f ( z ) f ( z ) q q 1 z D ˜ q f ( z ) f ( z ) + 2 q 1 1 = 2 q 1 ( k + 1 ) γ n = 2 [ n ] ˜ q 1 a n z n q + q 1 + n = 2 q q 1 [ n ] ˜ q + 2 q 1 a n z n , 2 q 1 ( k + 1 ) γ n = 2 [ n ] ˜ q 1 a n q + q 1 n = 2 q q 1 [ n ] ˜ q + 2 q 1 a n .
The expression (41) is bounded above by 1.
2 q 1 ( k + 1 ) γ n = 2 [ n ] ˜ q 1 a n q + q 1 n = 2 q q 1 [ n ] ˜ q + 2 q 1 a n < 1 .
After some simple calculations, we have
n = 2 2 q 1 ( k + 1 ) [ n ] ˜ q 1 + γ q q 1 [ n ] ˜ q + 2 q 1 a n q + q 1 γ .
Hence, we complete the proof of Theorem 1. □
When q 1 and γ = 1 α with 0 α < 1 , we have the following known result (see [7]).
Corollary 1.
An analytic function f of the form (1) belongs to the class k- UST ( α ) if it satisfies the condition
n = 2 n ( k + 1 ) ( k + α ) a n 1 α ,
where 0 α < 1 and k 0 .
Inequality (23) gives the following corollary:
Corollary 2.
Let 0 k < , q 0 , 1 and γ C \ { 0 } . If the inequality
a n q + q 1 γ 2 q 1 ( k + 1 ) [ n ] ˜ q 1 + γ q q 1 [ n ] ˜ q + 2 q 1 , n 2 ,
holds for f ( z ) = z + a n z n , then k - UST ( q , q 1 , γ ) . In particular,
f ( z ) = z + q + q 1 γ 2 q 1 ( k + 1 ) [ 2 ] ˜ q 1 + γ q q 1 [ 2 ] ˜ q + 2 q 1 z 2 k - UST ( q , q 1 , γ )
and
a 2 = q + q 1 γ 2 q 1 ( k + 1 ) [ 2 ] ˜ q 1 + γ q q 1 [ 2 ] ˜ q + 2 q 1 .
Coefficient estimates for the class k- UST ( q , q 1 , γ ) are given in the next Theorem.
Theorem 2.
If f k - UST ( q , q 1 , γ ) and is of the form 1, then
a 2 2 q 1 Q 1 q 1 + q
and
a n j = 0 n 2 Q 1 [ j ] ˜ q q 1 + q [ j + 1 ] ˜ q φ j f o r n 3 ,
where Q 1 and φ j are defined by (5) and (29).
Proof. 
Let
q 1 + q z D ˜ q f ( z ) f ( z ) q q 1 z D ˜ q f ( z ) f ( z ) + 2 q 1 = p ( z ) .
After some simple simplification of Equation (27), we have
q 1 + q z + n = 2 q 1 + q [ n ] ˜ q a n z n = q 1 + q z + n = 2 q q 1 [ n ] ˜ q + 2 q 1 a n z n 1 + n = 1 c n z n .
Equating coefficients of z n on both sides, we have
2 q 1 [ n ] ˜ q 1 a n = j = 1 n 1 [ j 1 ] ˜ q ( q q 1 ) + 2 q 1 a n j c j , a 1 = 1 .
This implies that
a n 1 2 q 1 [ n ] ˜ q 1 j = 1 n 1 [ j 1 ] ˜ q ( q q 1 ) + 2 q 1 a n j c j .
By using Lemma 3, we have
a n Q 1 q 1 + q [ n ] ˜ q 1 j = 1 n 1 [ j 1 ] ˜ q ( q q 1 ) + 2 q 1 a j ,
a n Q 1 q 1 + q [ n ] ˜ q 1 j = 1 n 1 φ j 1 a j ,
where
φ j 1 = [ j 1 ] ˜ q ( q q 1 ) + 2 q 1 .
Now we prove that
Q 1 q 1 + q [ n ] ˜ q 1 j = 1 n 1 φ j 1 a j j = 0 n 2 Q 1 [ j ] ˜ q q 1 + q [ j + 1 ] ˜ q φ j .
For this, we use the induction method. For n = 2 from (28), we have
a 2 2 q 1 Q 1 q 1 + q , φ 0 = 2 q 1
From (26), we have
a 2 2 q 1 Q 1 q 1 + q , φ 0 = 2 q 1 .
For n = 3 , from (28), we have
a 3 Q 1 q 1 + q [ 3 ] ˜ q 1 φ 0 + φ 1 a 2 , 2 q 1 Q 1 q 1 + q [ 3 ] ˜ q 1 1 + Q 1 , φ 1 = q 1 + q .
From (26), we have
a 3 Q 1 φ 0 q 1 + q Q 1 [ 1 ] ˜ q q 1 + q [ 2 ] ˜ q φ 1 , Q 1 φ 0 q 1 + q Q 1 + [ 1 ] ˜ q q 1 + q [ 2 ] ˜ q φ 1 , = Q 1 φ 1 q 1 + q [ 2 ] ˜ q Q 1 φ 0 q 1 + q + φ 0 q 1 + q , = Q 1 φ 1 q 1 + q [ 2 ] ˜ q Q 1 φ 0 q 1 + q + φ 0 q 1 + q , = 2 q 1 Q 1 q 1 + q [ 2 ] ˜ q Q 1 + 1 .
Let the hypothesis be true for n = m . From (28), we have
a m Q 1 q 1 + q [ m ] ˜ q 1 j = 1 m 1 φ j 1 a j .
From (26), we have
a m j = 0 m 2 Q 1 [ j ] ˜ q q 1 + q [ j + 1 ] ˜ q φ j , n 2 , j = 0 m 2 Q 1 + [ j ] ˜ q q 1 + q [ j + 1 ] ˜ q φ j , n 2 .
By the induction hypothesis, we have
Q 1 q 1 + q [ m ] ˜ q 1 j = 1 m 1 φ j 1 a j j = 0 m 2 Q 1 + [ j ] ˜ q q 1 + q [ j + 1 ] ˜ q φ j .
Multiplying Q 1 + [ m ] ˜ q 1 q 1 + q [ m ] ˜ q 1 on both sides of (31), we have
j = 0 m 2 Q 1 + [ j ] ˜ q q 1 + q [ j + 1 ] ˜ q φ j , Q 1 + [ m ] ˜ q 1 q 1 + q [ m ] ˜ q 1 Q 1 q 1 + q [ m ] ˜ q 1 j = 1 m 1 φ j 1 a j , = Q 1 q 1 + q [ m ] ˜ q 1 Q 1 q 1 + q [ m ] ˜ q 1 + 1 j = 1 m 1 φ j 1 a j , Q 1 q 1 + q [ m ] ˜ q 1 q a m + j = 1 m 1 φ j 1 a j , = Q 1 q 1 + q [ m ] ˜ q 1 j = 1 m φ j 1 a j .
That is
Q 1 q 1 + q [ m ] ˜ q 1 j = 1 m φ j 1 a j j = 0 m 2 Q 1 + [ j ] ˜ q q 1 + q [ j + 1 ] ˜ q φ j ,
which shows that inequality (31) is true for n = m + 1 . Hence, the proof of Theorem 2 is now completed. □
Corollary 3.
If f ( z ) k - UST ( γ ) and is of the form 1, then
a n j = 0 n 2 Q 1 j ( j + 1 ) f o r n 3 .
For q 1 , Kanas and Wisniowska proved Corollary (3) in [4].
In the next Theorem, we state and prove the Fekete–Szegö-type result for our defined function class k- UST ( q , q 1 , γ ) .
Theorem 3.
Let 0 k < , q ( 0 , 1 ) be fixed, and let f ( z ) k - UST ( q , q 1 , γ ) and be of the form (1). Then for a complex number μ,
a 3 μ a 2 2 Q 1 2 q 1 + q [ 3 ] ˜ q 1 max 1 , 2 v 1 ,
where v is given by (37).
Proof. 
If f ( z ) k - UST ( q , q 1 , γ ) , then we have
J ( q , q 1 , f ( z ) ) p k , q , q 1 , γ ˜ ( z )
and if there exists a Schwarz function w ( z ) , we have
q 1 + q z D q f ( z ) f ( z ) q q 1 z D q f ( z ) f ( z ) + 2 q 1 = p k , q , q 1 , γ ˜ ( w ( z ) ) .
Let the function h ( z ) P , defined by:
h ( z ) = 1 + w ( z ) 1 w ( z ) ,
this gives
w ( z ) = c 1 2 z + 1 2 c 2 c 1 2 2 z 2 +
and
p k , q , q 1 , γ ˜ ( w ( z ) ) = 1 + q 1 Q 1 c 1 q 1 + q z + q 1 q 1 + q ϝ 1 q , q 1 z 2 + ,
where
ϝ 1 q , q 1 = Q 2 c 1 2 2 + ( c 2 c 1 2 2 ) Q 1 ( q 1 q ) Q 1 2 c 1 2 2 .
Now, from L.H.S of (33), we have
q 1 + q z D q f ( z ) f ( z ) q q 1 z D q f ( z ) f ( z ) + 2 q 1 = 1 + 2 q 1 [ 2 ] ˜ q 1 q 1 + q a 2 z + ϝ 2 q , q 1 z 2 + . . . ,
where
ϝ 2 q , q 1 = 2 q 1 [ 3 ] ˜ q 1 a 3 2 q 1 q 1 + q [ 2 ] ˜ q 1 q q 1 [ 2 ] ˜ q + 2 q 1 a 2 2 .
By using (34) and (35) in (33), we obtain
a 2 = Q 1 c 1 2 [ 2 ] ˜ q 1
and
a 3 = 1 2 q 1 + q [ 3 ] ˜ q 1 ϝ 1 q , q 1 + q q 1 [ 2 ] ˜ q + 2 q 1 Q 1 2 c 1 2 2 [ 2 ] ˜ q 1 .
For any complex number μ we have
a 3 μ a 2 2 = Q 1 2 q 1 + q [ 3 ] ˜ q 1 c 2 v c 1 2 ,
where
v = 1 2 1 Q 2 Q 1 + ( q 1 q ) Q 1 ϝ 3 q , q 1
and
ϝ 3 q , q 1 = q q 1 2 q + 2 q 1 Q 1 [ 2 ] ˜ q 1 + μ q 1 + q [ 3 ] ˜ q 1 Q 1 [ 2 ] ˜ q 1 2 .
Now by using Lemma 4 on 36 , we have
a 3 μ a 2 2 Q 1 2 q 1 + q [ 3 ] ˜ q 1 max 1 , 2 v 1 .
Hence, we complete the proof of Theorem 3. □
Next we investigate the necessary and sufficient conditions for f ( z ) of the form (17) to be in the class k- UST ( q , q 1 , γ ) .
Theorem 4.
Let k [ 0 , ) , q 0 , 1 and γ C \ { 0 } . A function f ( z ) of the form (17) will belong to the class k- UST ( q , q 1 , γ ) which can be expressed as:
n = 2 2 q 1 ( k + 1 ) [ n ] ˜ q 1 + γ q q 1 [ n ] ˜ q + 2 q 1 a n q + q 1 γ .
The result is sharp for the function
f ( z ) = z q + q 1 γ 2 q 1 ( k + 1 ) [ n ] ˜ q 1 + γ q q 1 [ n ] ˜ q + 2 q 1 z n .
Proof. 
In view of Theorem 1, it remains to prove the necessity.
If f z k - UST ( q , q 1 , γ ) , then infect that ( z ) z ; for any z, we have
1 + 1 γ q + q 1 n = 2 2 q 1 [ n ] ˜ q 1 a n z n 1 1 n = 2 1 q + q 1 q q 1 n q + 2 q 1 a n z n 1 k γ q + q 1 n = 2 2 q 1 [ n ] ˜ q 1 a n z n 1 1 n = 2 1 q + q 1 q q 1 n q + 2 q 1 a n z n 1 .
Letting z 1 along the real axis, we obtain the desired inequality (38). Hence we complete the proof of Theorem 4. □
Corollary 4.
Let the function f ( z ) of the form (17) be in the class k- UST ( q , q 1 , γ ) . Then
a n q + q 1 γ 2 q 1 ( k + 1 ) [ n ] ˜ q 1 + γ q q 1 [ n ] ˜ q + 2 q 1 , n 2 .
Corollary 5.
Let the function f ( z ) of the form (17) be in the class k- UST ( q , q 1 , γ ) . Then
a 2 = q + q 1 γ 2 q 1 ( k + 1 ) [ 2 ] ˜ q 1 + γ q q 1 [ 2 ] ˜ q + 2 q 1 .
Theorem 5.
Let k [ 0 , ) , q 0 , 1 and γ C \ { 0 } and let
f 1 ( z ) = z ,
and
f n ( z ) = z R n , q z n , n 3 .
Then f k - UST ( q , q 1 , γ ) , if and only if f can be expressed in the form of
f ( z ) = n = 1 λ n f n ( z ) , λ n > 0 , and n = 1 λ n = 1 ,
where R n , q is given by (44).
Proof. 
Suppose that
f ( z ) = n = 1 λ n f n ( z ) = λ 1 f 1 ( z ) + n = 2 λ n f n ( z ) , = λ 1 f 1 ( z ) + n = 2 λ n z R n , q z n , = λ 1 z + n = 2 λ n z n = 2 λ n R n , q z n , = n = 1 λ n z n = 2 λ n R n , q z n , = z n = 2 λ n R n , q z n ,
where
R n , q = q + q 1 γ 2 q 1 ( k + 1 ) [ n ] ˜ q 1 + γ q q 1 [ n ] ˜ q + 2 q 1 .
Then
n = 2 λ n R n , q × 1 R n , q = n = 2 λ n = n = 1 λ n λ 1 = 1 λ 1 1 ,
and we find k- UST ( q , q 1 , γ ) .
Conversely, suppose that k- UST ( q , q 1 , γ ) . Since
a n R n , q ,
we can set
λ n = 1 R n , q a n ,
and
λ 1 = 1 n = 2 λ n .
Then
f ( z ) = z + n = 2 a n z n = z + n = 2 λ n R n , q z n , = z + n = 2 λ n ( z + f n ( z ) ) = z + n = 2 λ n z + n = 2 λ n f n ( z ) , = 1 n = 2 λ n z + n = 2 λ n f n ( z ) = λ 1 z + n = 2 λ n f n ( z ) = n = 1 λ n f n ( z ) .
The proof of Theorem 5 is complete. □
Theorem 6.
Let k [ 0 , ) , q ( 0 , 1 ) , z = r < 1 and γ C \ { 0 } . Let f of the form (17) be in the class k UST ( q , q 1 , γ ) . Then
r R 2 , q r 2 f ( z ) r + R 2 , q r 2 .
Equality in (45) is attained for the function f given by the formula
f ( z ) = z + R 2 , q z 2 ,
where
R 2 , q = q + q 1 γ 2 q 1 ( k + 1 ) [ 2 ] ˜ q 1 + γ q q 1 [ 2 ] ˜ q + 2 q 1 .
Proof. 
Since f k - UST ( q , q 1 , γ ) , in view of Theorem 4, we find
2 q 1 ( k + 1 ) [ 2 ] ˜ q 1 + γ q q 1 [ 2 ] ˜ q + 2 q 1 n = 2 a n n = 2 2 q 1 ( k + 1 ) [ n ] ˜ q 1 + γ q q 1 [ n ] ˜ q + 2 q 1 a n q + q 1 γ .
This gives
n = 2 a n R 2 , q .
Therefore
f ( z ) z + n = 2 a n z n r + R 2 , q r 2 ,
and
f ( z ) z n = 2 a n z n r R 2 , q r 2 .
By letting r 1 , we get the required result. Hence, the proof of Theorem 6 is complete. □
Theorem 7.
Let k [ 0 , ) , q ( 0 , 1 ) , z = r < 1 and γ C \ { 0 } . Let f be of the form (17) in the class k- UST ( q , q 1 , γ ) . Then
1 2 R 2 , q r f ( z ) 1 + 2 R 2 , q r .
Proof. 
Differentiating f and using triangle inequality for the modulus, we obtain
f ( z ) 1 + n = 2 n a n z n 1 1 + r n = 2 n a n ,
and
f ( z ) 1 n = 2 n a n z n 1 1 r n = 2 n a n .
Assertion (47) follows from (48) and (49); in view of the rather simple consequence, we get the following inequality
n = 2 n a n 2 R 2 , q .
Hence, proof of Theorem 7 is complete. □
Theorem 8.
Under convex linear combination, the class k- UST ( q , q 1 , γ ) is closed.
Proof. 
Let f ( z ) and g ( z ) be in class k- UST ( q , q 1 , γ ) . Suppose f ( z ) is given by (17) and
g ( z ) = z n = 2 d n z n ,
where a n , d n 0 .
It is sufficient to show that for 0 λ 1 , the function
H ( z ) = λ f ( z ) + ( 1 λ ) g ( z ) k - UST ( q , q 1 , γ ) .
From (17), (50) and (51), we have
H ( z ) = z n = 2 λ a n + 1 λ d n z n .
As we know that f and g are in class k- UST ( q , q 1 , γ ) 0 λ 1 , by using Theorem 4, we obtain
n = 2 2 q 1 ( k + 1 ) [ n ] ˜ q 1 + γ q q 1 [ n ] ˜ q + 2 q 1 λ a n + 1 λ d n ( 1 + q ) γ .
Again, by Theorem 4 and inequality (53), we have H ( z ) k - UST ( q , q 1 , γ ) . Hence, the proof of Theorem 8 is complete. □

4. Conclusions

In this paper, motivated significantly by a number of recent works, we used the concept of symmetric quantum calculus and conic regions to define a new domain Ω k , q , q 1 , γ ˜ , which generalizes the symmetric conic domains. By using a certain generalized symmetric conic domain Ω k , q , q 1 , γ ˜ , we defined and investigated a new subclass of normalized analytic q-starlike functions in the open unit disk E, and we have successfully derived several properties and characteristics of a newly defined subclass of analytic functions. For the verification and validity of our main results, we have also pointed out relevant connections of our main results with those in several earlier related works on this subject.
To conclude our present investigation, we would like to remark that one may attempt the results presented in this paper for different subclasses of analytic functions in different domains. In particular, one may define a new subclass of symmetric q-starlike functions associated with this newly defined domain and can obtain the same results.

Author Contributions

The authors have equally contributed to accomplish this research work. All authors have read and agreed to the published version of the manuscript.

Funding

This research receive no external funding.

Institutional Review Board Statement

Not applicable.

Informed Consent Statement

Not applicable.

Data Availability Statement

Not applicable.

Conflicts of Interest

The authors agree with the contents of the manuscript, and there are no conflict of interest among the authors.

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Khan, S.; Khan, N.; Hussain, A.; Araci, S.; Khan, B.; Al-Sulami, H.H. Applications of Symmetric Conic Domains to a Subclass of q-Starlike Functions. Symmetry 2022, 14, 803. https://0-doi-org.brum.beds.ac.uk/10.3390/sym14040803

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Khan S, Khan N, Hussain A, Araci S, Khan B, Al-Sulami HH. Applications of Symmetric Conic Domains to a Subclass of q-Starlike Functions. Symmetry. 2022; 14(4):803. https://0-doi-org.brum.beds.ac.uk/10.3390/sym14040803

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Khan, Shahid, Nazar Khan, Aftab Hussain, Serkan Araci, Bilal Khan, and Hamed H. Al-Sulami. 2022. "Applications of Symmetric Conic Domains to a Subclass of q-Starlike Functions" Symmetry 14, no. 4: 803. https://0-doi-org.brum.beds.ac.uk/10.3390/sym14040803

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