1. Introduction and Preliminaries
Let
denote the collection of complex-valued functions that are analytic on the open unit disk,
We define
as the subset of
consisting of functions that satisfy the normalization condition
where
. When
, this family coincides with the classical class of normalized analytic functions
.
Definition 1 ([
1]).
Given two functions f and g analytic in , the function f is subordinate to g in , denoted byif there exists a Schwarz function , analytic in , with and , such that The study of analytic and multivalent function classes has a long and rich history, beginning with classical subclasses such as starlike and convex functions and evolving through the introduction of various operator-based frameworks. A key milestone was Janowski’s subordination approach, which provided a flexible way to define families of analytic functions via transformations associated with conic domains. Subsequent works by Aouf (see [
2]), Hayami–Owa (see [
3]), and others refined these ideas for multivalent functions, while Srivastava and coauthors (see [
4]) developed generalized differential and integral operators that allowed a systematic treatment of broader subclasses. Over the years, the focus has increasingly shifted toward constructing function classes that are stable under differential or integral operators, admit sharp coefficient estimates, and display inclusion, distortion, and neighborhood properties analogous to their classical counterparts. Motivated by these developments, the present paper incorporates higher-order differential operators in the framework of
q-calculus, aiming to extend and unify several existing families of analytic functions through Janowski-type subordination.
In recent years,
q-calculus has emerged as a focal area of research owing to its broad applications across many branches of mathematics and key areas of physics. The
q-derivative has proved to be an essential tool for analyzing numerous subclasses of analytic functions, while the
q-difference operator plays a central role in the theory of basic hypergeometric series and is frequently used in quantum physics (see [
5,
6]). The notion of
q-starlike functions dates to 1990 with foundational work by Ismail and coauthors (see [
7]). A systematic framework for embedding
q-calculus into Geometric Function Theory was later developed by Srivastava, notably via generalized basic hypergeometric functions (see [
4]). Since then, many contributions have enriched the subject. For example, Arif and collaborators [
8] introduced the Noor integral operator in the
q-calculus setting via convolution methods, thereby generating new subclasses of analytic functions. Parallel investigations [
9] examined generalized differential operators within
q-calculus and their action on newly introduced families of analytic functions. Wongsai Jai and Sukantamala [
10] carried out an in-depth study of subclasses defined by
q-starlikeness, highlighting several analytic properties. Srivastava and coauthors (see [
11]) broadened the scope by incorporating
q-starlike functions associated with conic regions, and subsequent works explored interactions with Janowski functions (see [
12,
13]). More recently, Srivastava’s comprehensive survey (see [
14]) synthesized these developments, discussed extended
q-analogues in fractional contexts, emphasized their connections to
q-differential operators, and outlined their role in geometric function theory. This survey now serves as a central reference for researchers active in the field.
Several recent works have highlighted the role of
q-calculus in geometric function theory, particularly through the use of higher-order
q-derivatives, fractional operators, and Janowski-type functions (see for example [
15,
16,
17,
18]).
We now recall certain notions and symbols from the q-calculus that will be essential in the subsequent analysis.
The idea underlying
q-analogues, also referred to as
q-extensions of classical results, is encapsulated in the identity,
The expression
is commonly called the basic number and denoted by
.
The corresponding
q-factorial is defined as
As , q-analogues recover their classical forms; in particular, .
It is worth noting the basic-number relation
which follows directly from the definition
.
Jackson, in [
19,
20], introduced the
q-derivative operator
acting on functions
by
In the limit
,
reduces to the ordinary derivative
.
For the monomial
, one has
and consequently, as
,
Using Equation (
5), we obtain
The operator
satisfies the following rules for
f,
g and
:
The
q-integral of
f over
is given by (see [
19])
provided the series converges.
In the limit
, this reduces to the usual integral
Higher-order
q-derivatives are defined recursively by
Explicitly, the
q-derivative of the function
of order
r is given by
for
and
.
The definition of the
q-Gamma function
is given by
which satisfies the following fundamental properties:
and
where
and the
q-factorial
is defined in Equation (
3).
We next revisit several key definitions related to fractional q-calculus operators for complex-valued functions .
Definition 2 ([
21]).
The fractional q-integral of order for the function f is defined bywith analytic in a simply connected region of the complex plane that contains the origin. Here denotes the standard fractional q-shifted kernel used in fractional q-calculus, taken on the branch for which is real whenever . Throughout, we assume the principal branch and that the resulting integrals/series are absolutely convergent for . Definition 3 ([
21]).
The fractional q-derivative of order α for the function f is defined by The theory of univalent and multivalent functions has seen major developments through the introduction of various subclasses defined by analytic, geometric, or operator-based properties. A fruitful approach involves the use of differential operators and subordination principles to describe starlike or convex function classes. When extended to the framework of q-calculus, these ideas give rise to discrete analogues such as q-starlike or q-convex functions.
For
and
, Aouf [
22] defined the class
, which represents a subclass of the family
and comprises functions represented by
with the property that
Aouf (see [
22]) introduced the subclass
of multivalent quasi-starlike functions defined by a subordination involving the derivative
and the fractional transformation of Janowski-type. Later, authors like Srivastava et al. (see [
23,
24,
25]) developed further classes using higher-order
q-derivatives and generalized subordination functions.
To make the presentation self-contained, we summarize below the main symbols, operators, and parameters used throughout the paper (
Table 1).
In this work, we address the absence of a unified framework for Janowski-type subclasses of analytic functions involving higher-order q-derivatives, encompassing both positive and negative coefficient cases. By employing higher-order q-derivative operators and Janowski subordination, we define two new normalized q-classes within the standard family , which encompass subclasses with both positive and negative coefficients, thereby extending and unifying several classical families in geometric function theory. Sharp coefficient inequalities are obtained, together with structural properties such as invariance under arithmetic and weighted means, parameter monotonicity, and distortion bounds. We also establish Goodman–Ruscheweyh–type neighborhood inclusions and apply the results to fractional q-calculus, particularly to the q-Jung–Kim–Srivastava operator, with all main theorems reducing to known results as .
Let us define the generalized Janowski-type function as follows:
where
and
,
.
Definition 4. Let , with , , , and with . A function is said to belong to the class ifthat is, there exists a Schwarz function , analytic in with and , such thatwith given by Equation (8). Remark 1. Because the series representations of and are absolutely and uniformly convergent on compact subsets of , all termwise operations are justified.
Remark 2. Throughout, we assume, without repeated mention, that the following conditions hold: , , with , , , , and with .
Remark 3. The class reduces to several known subclasses of multivalent functions for particular choices of parameters:
If , , and , then reduces to the class introduced by Aouf (see [22]) where If , , and , then becomes the class of n-valent starlike functions of order β, .
If , , and , then specializes to the class investigated by Hayami and Owa [3]. If , , , then reduces to the class proposed by Polatoglu et al. [26]. If , , , and , then reduces to the subclass considered by Janowski [27] and was further studied by Goel and Mehrok [28]. If , , , , , then reduces to .
If , , , , and , then reduces to .
We denote by
the subclass of
consisting of all functions having negative coefficients, namely
We furthermore introduce
.
Remark 4. By assigning specific values to the parameter values, we recover several well-known subclasses of analytic functions in with negative coefficients:
If , and , then becomes the class introduced and studied by Aouf (see [2]). If , , , and , then reduces to the class proposed by Sekine and Owa (see [29]). If , , , , , , , then reduces to the class investigated by Kim and Lee (see [30]).
For , we denote the class by .
Lemma 1 ([
31]).
Let , then 2. Coefficient Characterizations and Fundamental Properties of the Class
In this section, we derive a coefficient inequality that characterizes functions belonging to the class . Building on this characterization, we establish sharp coefficient bounds and investigate inclusion properties of various subclasses. Furthermore, we examine the behavior of these classes under weighted and arithmetic mean operations, prove several distortion theorems, and derive related corollaries. These results provide a unified framework for analyzing geometric properties of q-multivalent functions with negative coefficients.
Theorem 1. Suppose is analytic in the unit disk . The function f belongs to the class if and only ifwhereand Proof. The subordination condition defining the class
can be written equivalently as
Using Equation (
4) and substituting the series expansion for
and
, we obtain
Taking
and applying the triangle inequality to numerator and denominator, we get
which leads directly to Equation (
11), where
and
C are given by Equations (
12) and (
13).
In the reverse direction, let
belong to class
. So, we have
Fix
and write
with
. To pass from the complex inequality to the real-part bound, we choose
z such that the transformed ratio is real, and use the inequality
. We have
The limit as
is then justified by dominated convergence, owing to the absolute and uniform convergence of the underlying series. So, we obtain
and the proof is now complete. □
Remark 5. Since the class is a subset of it suffices for the function to satisfy Equation (11) of the previous theorem in order to be a member of . In order to illustrate the definition of the class , we provide an explicit example for specific parameter choices.
Example 1. Let , , , , , , . We haveHence , where C is given by Equation (13). From Theorem 1, the extremal function corresponding to iswhereTherefore,belongs to the class and satisfies Equation (11) exactly. Corollary 1. Let be given by Equation (10). If , then for every the coefficient boundholds, where . This estimate is sharp in each coordinate: for every fixed j, equality is attained by the extremal function For
,
and
in Theorem 1, we obtain the following result previously obtained by Aouf (see [
2])
Corollary 2. The function belongs to the class if and only if For in Theorem 1, we obtain the following result:
Corollary 3. Let analytic in the unit disk . The function f belongs to the class if and only ifwhere C is given by Equation (13) and Theorem 2. Let the function belong to the class , where . Then Proof. Applying Corollary 3, Equation (
15) yields
hence Equation (
16) follows immediately. □
Utilizing Theorem 1, we can establish that the class remains invariant under both weighted and arithmetic means.
Theorem 3. Letbe two functions in the class . For any , defineThen . Proof. For ease of notation, set:
where
is given by Equation (
12) and
C is given by Equation (
13). By the coefficient characterization Theorem 1, the functions
if and only if
In terms of its series representation,
takes the form:
Since
, we have
and
, hence
and the required sign structure of the coefficients is preserved.
Using linearity and Equation (
18),
Therefore the characterization Equation (
11) holds for the coefficients of
, and thus
. This proves that the class
is closed under the weighted mean. □
Theorem 4. Letbe functions in the class . Then their arithmetic meanalso belongs to . Proof. The function
G can be expressed in the same negative-coefficients series representation:
Clearly
, so the coefficient pattern required by the subclass is preserved.
In view of Equations (
17) and (
13) and by Theorem 1, a function
belongs to
if and only if
Since each
, we have for every
,
Using linearity and the definition of
,
Thus Equation (
19) holds for
G, and by Theorem 1 we conclude
. This proves closure under arithmetic means. □
The next theorem establishes a monotonicity property with respect to the parameters.
Theorem 5. Let and . Then Proof. Let
. From Equation (
9), we have
From
and
, we obtain
The middle inequality in the chain follows because the expression
increases with
M and decreases with
.
In view of Lemma 1, we get
Hence,
. □
In the sequel, we establish the following distortion theorems.
Theorem 6. If , then for , ,where C is given in Equation (13) andThe bounds in Equation (20) are sharp and are achieved by the function defined byat and . Proof. By Theorem 1, one readily gets
and thus
A similar estimate yields the lower bound.
The extremal function
attains equality in (
20) at
(for the upper bound) and
(for the lower bound), since in these cases
. This confirms the sharpness of both bounds.
Hence, the proof is finished. □
For
,
and
, we obtain the following result previously obtained by Aouf (see [
2]).
Corollary 4. If , then for , , For , we get:
Corollary 5. If and , then for , ,where C is given in Equation (13) andThe bounds in Equation (23) are sharp and are achieved byat and . The proof of the next result is analogous to that of Theorem 6, and is therefore omitted.
Theorem 7. If , then for , ,andwhere C and are given by Equations (13) and (21). The bounds in Equations (26) and (27) are sharp and are achieved by the function specified by Equation (20). For
,
and
, we obtain the following result previously obtained by Aouf (see [
2]).
Corollary 6. If , then for , ,For , we get: Corollary 7. If and , then for , ,where C is given in Equation (13) and is given in Equation (24). The bounds are sharp and are achieved by Equation (25). Example 2. Let’s takeThen , , hencewhere C is given by (13). We also record the basic q-numbers (with ):We give now coefficient bounds from Theorem 1 (for ): For , Theorem 1 giveswith given by Equation (12). For : Hence,For : Hence,Distortion estimate at . For ,Thus,where and C are given by Equations (12) and (13). Therefore, for and ,Note. The distortion theorem requires (satisfied since ) and . For this parameter choice, the last quantity equals ; if one chooses , the hypothesis is strictly satisfied.