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Some applications of q-difference operator involving a family of meromorphic harmonic functions
Advances in Difference Equations volume 2021, Article number: 471 (2021)
Abstract
In this paper, we establish certain new subclasses of meromorphic harmonic functions using the principles of q-derivative operator. We obtain new criteria of sense preserving and univalency. We also address other important aspects, such as distortion limits, preservation of convolution, and convexity limitations. Additionally, with the help of sufficiency criteria, we estimate sharp bounds of the real parts of the ratios of meromorphic harmonic functions to their sequences of partial sums.
1 Introduction and definitions
Univalent harmonic functions are a new research area that was initially developed by Clunie and Sheil-Small [15]; see also [40]. The significance of such functions is attributed to their usage in the analysis of minimal surfaces and in problems relevant to applied mathematics. Hengartner and Schober [18] introduced and analyzed some specific types of harmonic functions in the region \(\widetilde{\mathfrak{D}}\mathbb{=} \{ z\in \mathbb{C} : \vert z \vert >1 \} \). They proved that a harmonic complex-valued sense-preserving univalent mapping f defined in \(\widetilde{\mathfrak{D}}\) and obeying \(f ( \infty ) =\infty \) must satisfy the following representation:
where
with \(0\leq \vert \mu _{2} \vert < \vert \mu _{1} \vert \) and \(A\in \mathbb{C} \). In 1999, Jahangiri and Silverman [26] gave adequate coefficient criteria for functions of type (1.1) to be univalent. They also provided necessary and sufficient coefficient criteria within certain constraints for functions to be harmonic and starlike. Using this idea, the authors of [24] contributed a certain family of harmonic close-to-convex functions involving the Alexander integral transform. In 2000, Jahangiri [22] and Murugusundaramoorthy [35, 36] analyzed the families of meromorphic harmonic function in \(\widetilde{\mathfrak{D}}\). In [12, 14] the authors used the technique developed by Zou and his coauthors in [55] to examine the natures of meromorphic harmonic starlike functions with respect to symmetrical conjugate points in the punctured disc \(\mathfrak{D}^{\ast }\mathbb{=} \{ z\in \mathbb{C} :0< \vert z \vert <1 \} =\mathfrak{D} \backslash \{0\}\). Particularly, in [14] a sharp approximation of the coefficients and a structural description of these functions are also determined. To understand the basics in a more clear way, we denote by \(\mathcal{H}\) the family of harmonic functions f that can be represented in the series form
where \(\mathfrak{h}\) and \(\mathfrak{g}\) are holomorphic functions in \(\mathfrak{D}^{\ast }\) and \(\mathfrak{D}\) of the form
and
Also, let us denote by \(\mathcal{M}_{\mathcal{H}}\) the set of complex-valued functions \(f\in \mathcal{H}\) that are sense preserving and univalent in \(\mathfrak{D}^{\ast }\). Clearly, if \(\mathfrak{g} ( z ) \equiv 0\) \(( z\in \mathfrak{D} ) \), then \(\mathcal{M}_{\mathcal{H}}\) matches with the collection \(\mathcal{M}\) of holomorphic univalent normalized functions in \(\mathfrak{D}\). The above foundational papers opened a new door for the researchers to add some input in this area of function theory. In this regard, we consider the collections of meromorphic harmonic starlike and meromorphic harmonic convex functions in \(\mathfrak{D}^{\ast }\)
and
where the notation ≺ shows the familiar subordination between the holomorphic functions, and
Furthermore, many subfamilies of meromorphic harmonic functions have also been established by some well-known researchers; for example, see Bostanci [11], Bostanci and Öztürk [13], Öztürk and Bostanci [38], Wang et al. [54], Al-dweby and Darus [3], Al-Shaqsi and Darus [4], Ponnusamy and Rajasekaran [39], Ahuja and Jahangiri [2], Al-Zkeri and Al-Oboudi [5], Stephen et al. [53], and Khan et al. [32].
The investigation of q-calculus (q stands for quantum) fascinated and inspired many scholars due its use in various areas of the quantitative sciences. Jackson [20, 21] was among the key contributors of all the scientists who introduced and developed the q-calculus theory. Just like q-calculus was used in other mathematical sciences, the formulations of this idea are commonly used to examine the existence of various structures of function theory. The first paper in which a link was established between certain geometric nature of the analytic functions and the q-derivative operator is due to the authors [19]. For the usage of q-calculus in function theory, a solid and comprehensive foundation is given by Srivastava [43]. After this development, many researchers introduced and studied some useful operators in q-analog with applications of convolution concepts. For example, Kanas and Răducanu [27] established the q-differential operator and then examined the behavior of this operator in function theory. For more applications of this operator, see [1, 7, 17]. This operator was generalized further for multivalent analytic functions by Arif et al. [8] and later studied in [30, 41, 51]. Analogous to q-differential operator Arif et al. [9] and Khan et al. [33] contributed the integral operators for analytic and multivalent functions, respectively. Similarly, in [6] the authors developed and analyzed operators in q-analog for meromorphic functions. Also, see the survey-type paper [44] on quantum calculus and its applications. In 2021, Srivastava, Arif, and Raza [46] introduced and studied a generalized convolution q-derivative operator for meromorphic harmonic functions. Using these operators, many researchers contributed some good papers in this direction in geometric function theory; see [16, 23, 25, 28, 29, 31, 37, 45, 50, 52].
Definition 1.1
Let \(q\in ] 0,1 [ \). Then the q-analog derivative of f is
See also [10, 48, 49], and [47] for some recent applications of the q-difference operators in the theory of q-series and q-polynomials.
By means of (1.2) and (1.4) we obtain
where
To prevent repetition, we will assume, unless otherwise stated, that
Definition 1.2
By \(\mathcal{MS}_{\mathcal{H}}^{\ast } ( q,L,M ) \) we denote the set of functions \(f\in \mathcal{M}_{\mathcal{H}}\) such that
where
Similarly, we denote
In this paper, we learn some nice properties for the currently established families including distortion limits, univalency criteria, partial-sum problems, sufficiency criteria, convexity conditions, and preserving convolutions.
2 Necessary and sufficient conditions
Theorem 2.1
If \(f\in \mathcal{H}\) is described by the series of the form (1.2) and if
then \(f\in \mathcal{MS}_{\mathcal{H}}^{\ast } ( q,L,M ) \) with
Proof
If \(f ( z ) =\frac{1}{z}\), then we have \(\mathfrak{h} ( z ) =\frac{1}{z}\) and \(\mathfrak{g} ( z ) =0\). This implies that
Hence by the result of Lewy [34] the function f in \(\mathfrak{D}^{\ast }\) is locally univalent and orientation-preserving. Now we show that f is univalent in \(\mathfrak{D}^{\ast }\). Let \(z_{1},z_{2}\in \mathfrak{D}^{\ast }\) with \(z_{1}\neq z_{2}\). Then
To show that \(f\in \mathcal{MS}_{\mathcal{H}}^{\ast } ( q,L,M ) \), we have to establish that
It is easy to find that \(q\mathcal{D}_{\mathcal{H}}^{q}f ( z ) =-\frac{1}{z}\) and \(L-M>0\). This indicates that
Hence \(f\in \mathcal{MS}_{\mathcal{H}}^{\ast } ( q,L,M ) \). Now let \(f\in \mathcal{H}\) have be of the form (1.2), and let us choose \(n\geq 1\) such that \(a_{n}\neq 0\) or \(b_{n}\neq 0\). Also, by using
we have
Similarly, \(\frac{\rho _{n}}{L-M}\geq n\) for \(n\geq 1\). Thus using (2.1) together with the above evidence, we get
and therefore
Therefore by Lewy’s result [34] the function f in \(\mathfrak{D}^{\ast }\) is sense-preserving and locally univalent. Moreover, if \(z_{1,}z_{2}\in \mathfrak{D}^{\ast }\) with\(z_{1}\neq z_{2}\), then
Hence by (2.4) we have
This shows that f is univalent in \(\mathfrak{D}^{\ast }\), and thus \(f\in \mathcal{M}_{\mathcal{H}}\). Therefore \(f\in \mathcal{MS}_{\mathcal{H}}^{\ast } ( q,L,M ) \) if and only if there exists a holomorphic function u with \(u ( 0 ) =0\) and \(\vert u ( z ) \vert <1\) such that
or, alternatively,
To prove (2.5), it suffices to show that
for \(z\in \mathfrak{D}\). Putting \(\vert z \vert =r\) \(( 0< r<1 ) \), we attain
due inequality (2.1). Thus \(f\in \mathcal{MS}_{\mathcal{H}}^{\ast } ( q,L,M ) \). □
By substituting specific values of the parameters included in this result we obtain the following corollaries.
Corollary 2.2
Let \(f\in \mathcal{H}\) be of the form (1.2). If
with
then \(f\in \mathcal{MS}_{\mathcal{H}}^{\ast } ( q,1,-q ) \)
Proof
The result is obtained by setting \(L=1\) and \(M=-q\) in the last theorem. □
Corollary 2.3
Let \(f\in \mathcal{H}\) be given in (1.2). If
then \(f\in \mathcal{MS}_{\mathcal{H}}^{\ast } ( 1,1,-1 ) \).
Proof
Taking the limit as \(q\rightarrow 1-\) in the above corollary, we get the needed result. □
Influenced by Silverman’s paper [42], the set \(\vartheta ^{\lambda }\), \(\lambda \in \{ 0,1 \} \), of functions \(f\in \mathcal{H}\) of type (1.2) is now described as
Hence (1.2) and (1.3) give \(f ( z ) =\mathfrak{h} ( z ) + \overline{\mathfrak{g} ( z ) }\) with
Using the above facts, we now define the families
Let us now prove that condition (2.1) is also appropriate for \(f\in \mathcal{MS}_{\mathcal{H}_{\vartheta }}^{\ast } \).
Theorem 2.4
Let \(f\in \vartheta ^{0}\) have expansion (2.6). Then \(f\in \mathcal{MS}_{\mathcal{H}_{\vartheta }}^{\ast } ( q,L,M ) \) if and only if (2.1) is true.
Proof
To achieve the result, it is sufficient to determine that \(f\in \mathcal{MS}_{\mathcal{H}_{\vartheta }}^{\ast } ( q,L,M ) \) validates relationship (2.1). Let \(f\in \mathcal{MS}_{\mathcal{H}_{\vartheta }}^{\ast } ( q,L,M ) \). Then inequality (2.5) holds, that is, for \(z\in \mathfrak{D}^{\ast }\),
Setting \(z=r\) \(( r\in ( 0,1 ) ) \), we obtain
Obviously, in case of \(r\in ( 0,1 ) \), the left-hand side denominator of (2.7) cannot be zero. In addition, this is positive when \(r=0\). Thus, using (2.7), we get
It is straightforward that the partial-sum sequence \(\{ S_{n} \} \) attached with the series \(\sum_{n=1}^{\infty } ( \rho _{n} \vert a_{n} \vert + \sigma _{n} \vert b_{n} \vert ) \) is nondecreasing sequence, and by (2.8) it is bounded by \(( L-M ) \). So \(\{ S_{n} \} \) is a convergent sequence, and
which gives assumption (2.1). □
Example 2.5
Let us choose the function
Then we easily get
Thus \(T\in \mathcal{MS}_{\mathcal{H}_{\vartheta }}^{\ast } ( q,L,M ) \).
By using the above-mentioned theorem along with the notion of class \(\mathcal{MS}_{\mathcal{H}}^{c} ( q,L,M ) \) we can easily derive the following results.
Corollary 2.6
Let \(f\in \mathcal{H}\) be written in the form of Taylor expansion (1.2). If
then \(f\in \mathcal{MS}_{\mathcal{H}}^{c} ( q,L,M ) \).
Proof
From inequality (2.9), Theorem 2.1, and Alexander-type relation
we easily get the desired result. □
Corollary 2.7
Let \(f\in \vartheta ^{1}\) be written in the series form (2.6). Then \(f\in \mathcal{MS}_{\mathcal{H}_{\vartheta }}^{c} ( q,L,M ) \) if and only if inequality (2.9) is fulfilled.
Proof
Using relationship (2.10) and Theorem 2.4, we get the desired result. □
3 Investigation of partial-sum problems
In this section, we investigate problems of partial sums of certain meromorphic harmonic functions belonging to \(\mathcal{MS}_{\mathcal{H}}^{\ast } ( q,L,M ) \). We produce some new findings that connect the meromorphic harmonic functions with their partial-sum sequences. Let \(f=\mathfrak{h}+\) \(\overline{\mathfrak{g}}\) with \(\mathfrak{h}\) and \(\mathfrak{g}\) given in (1.3). Then the partial-sum sequences of f are specified by
Now we find sharp lower bounds for
and
Theorem 3.1
Let f have the form (1.2). If f fulfills (2.1), then
and
where
and
The findings above are best suited for the function
where \(\mathcal{I}_{t+1}\) is given by (3.4).
Proof
Let us represent
Inequality (3.1) will be acquired if we are able to show that Re\(\{ \Theta _{1} ( z ) \} >0\), and for this, we required to conclude that
Alternatively, we have the following inequalities:
if and only if
From (2.1) we have that it suffices to guarantee that the left-hand side of (3.6) is bounded above by
which is exactly equivalent to
and this is true because of (3.4). We observe that the function
offers the best possible outcome. We see for \(z=re^{i\frac{\pi }{t}}\) that
To examine (3.2), let us write
Then
if and only if
Inequality (3.7) is valid if the left-hand side of this inequality is bounded above by
and thus the proof is accomplished by using (2.1). □
Theorem 3.2
Let \(f=\mathfrak{h}+\) \(\overline{\mathfrak{g}}\), where \(\mathfrak{h}\) and \(\mathfrak{g}\) are given by (1.3). If f fulfills (2.1), then
and
where \(\mathcal{I}_{n}\) is given by (3.3), and
The equalities are achieved by considering the function
Proof
The proof for this specific outcome is similar to that of Theorem 3.1 and is thus omitted. □
Theorem 3.3
Let \(f=\mathfrak{h}+\overline{\mathfrak{g}}\) have the power series form (1.3). If f meets inequality (2.1), then
and
where \(\mathcal{I}_{n}\) is given by (3.3). The equalities are easily achieved by using (3.5).
Proof
To establish (3.12), let us consider
Therefore, to show inequality (3.12), it is sufficient to prove the inequality
Now recalling the left-hand side of the above-mentioned inequality, by easy calculations we get
Since we observe that from (2.1) that the denominator of the last inequality is positive. The right-hand side of the last inequality is also constrained by one if and only if the following inequality is maintained:
Eventually, to verify inequality (3.12), it suffices to show that the left-hand side of (3.14) is bounded above by
which is further analogous to
and this is true due to (3.10). Now let us choose
which delivers a sharp result. We observe that for \(z=re^{i\frac{\pi }{t}}\),
Similarly, we obtain (3.9). □
Theorem 3.4
Let \(f=\mathfrak{h}+\overline{\mathfrak{g}}\), where \(\mathfrak{h}\) and \(\mathfrak{g}\) are expressed by (1.3). If f meets (2.1), then
and
where \(\mathcal{I}_{n}\) is given by (3.3). The equalities are obtained for the function stated in (3.11).
Proof
The proof is very similar to that of Theorem 3.3 and is therefore omitted. □
4 Further properties of the class \(\mathcal{MS}_{\mathcal{H}_{\vartheta }}^{\ast } ( q,L,M ) \)
Theorem 4.1
If \(f\in \mathcal{MS}_{\mathcal{H}_{\vartheta }}^{\ast } ( q,L,M ) \), then for \(\vert z \vert =r\),
and
Proof
Let \(f=\mathfrak{h}+\overline{\mathfrak{g}}\) \(\in \mathcal{MS}_{\mathcal{H}_{\vartheta }}^{\ast } ( q,L,M ) \) with \(\mathfrak{h}\) and \(\mathfrak{g}\) of the series form (1.3). Then by Theorem 2.4 we have
This completes the proof of (4.1). By similar arguments we easily obtain (4.2). □
Theorem 4.2
A function \(f\in \mathcal{MS}_{\mathcal{H}_{\vartheta }}^{\ast } ( q,L,M ) \) if and only if
where
and \(\mathfrak{X}_{n}\mathfrak{,}\) \(\mathfrak{Y}_{n}\) ≥0 for \(n\in \mathbb{N}\) are such that
In particular, the points \(\{ \mathfrak{h}_{n} \} \), \(\{ \mathfrak{g}_{n} \} \) are called the extreme points of the closed convex hull of the set \(\mathcal{MS}_{\mathcal{H}_{\vartheta }}^{\ast } ( q,L,M ) \) denoted by \(clco\mathcal{MS}_{\mathcal{H}_{\vartheta }}^{\ast } ( q,L,M ) \).
Proof
Let f be specified by (4.3). Then from (4.4) we get
which by Theorem 2.4 indicates that \(f\in \mathcal{MS}_{\mathcal{H}_{\vartheta }}^{\ast } ( q,L,M ) \), since
Thus \(f\in clco\mathcal{MS}_{\mathcal{H}_{\vartheta }}^{\ast } ( q,L,M ) \). For the converse part, let \(f=\mathfrak{h}+\overline{\mathfrak{g}}\) \(\in \mathcal{MS}_{\mathcal{H}_{\vartheta }}^{\ast } ( q,L,M ) \). Put
Then utilizing (4.4) together with the hypothesis, we have
which is the needed form (4.3). Thus the proof of Theorem 4.2 is completed. □
Theorem 4.3
Let \(f_{1},f_{2}\) \(\in \mathcal{MS}_{\mathcal{H}_{\vartheta }}^{\ast } ( q,L,M ) \). Then \(f_{1}\ast f_{2}\in \mathcal{MS}_{\mathcal{H}_{\vartheta }}^{\ast } ( q,L,M ) \).
Proof
Let
and
Then
Now if \(f_{2}\) \(\in \mathcal{MS}_{\mathcal{H}_{\vartheta }}^{\ast } ( q,L,M ) \), then by Theorem 2.4 we have \(\vert A_{n} \vert \leq 1\) and \(\vert B_{n} \vert \leq 1\). Thus
By Theorem 2.4 this gives that \(f_{1}\ast f_{2}\in \mathcal{MS}_{\mathcal{H}_{\vartheta }}^{\ast } ( q,L,M ) \). □
Theorem 4.4
The family \(\mathcal{MS}_{\mathcal{H}_{\vartheta }}^{\ast } ( q,L,M ) \) is closed by a convex combination.
Proof
For \(k\in \mathbb{N}\), let \(f_{k}\in \mathcal{MS}_{\mathcal{H}_{\vartheta }}^{\ast } ( q,L,M ) \) be represented by
Then by (2.1) we have
For \(\sum_{k=1}^{\infty }\xi _{k}=1\), \(0\leq \xi _{k}<1\), the convex combination of \(f_{k}\) is
Then by Theorem 2.4 we can write
and so \(\sum_{k=1}^{\infty }\xi _{k}f_{k} ( z ) \in \mathcal{MS}_{\mathcal{H}_{\vartheta }}^{\ast } ( q,L,M ) \). □
5 Conclusion
Utilizing the principles of quantum calculus, we have added some new subfamilies of meromorphic harmonic mappings linked to a circular domain. We learned also certain important problems for the newly specified function families, namely necessary and sufficient conditions, problems for partial sums, distortion limits, convexity conditions, and convolution preserving. For these families, other problems, such as topological properties, fundamental mean inequality, and their implications are open problems for the scholars to investigate.
As pointed out in the survey-cum-expository review paper by Srivastava [44, p. 340], any attempt to produce the so-called \((p,q)\)-variation of the q-results, which we have presented in this paper, will be trivial and inconsequential because the additional parameter p is obviously redundant or superfluous.
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Khan, N., Srivastava, H.M., Rafiq, A. et al. Some applications of q-difference operator involving a family of meromorphic harmonic functions. Adv Differ Equ 2021, 471 (2021). https://doi.org/10.1186/s13662-021-03629-w
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DOI: https://doi.org/10.1186/s13662-021-03629-w