1. Introduction
The one parameter Mittag–Leffler function defined by
(1)
was introduced by Mittag–Leffler [1]. This function of complex variable is entire. The series defined by Equation (1) converges in when Consider that the function which generalizes the function is defined by(2)
It was introduced by Wiman [2] and was named as Mittag–Leffler type function. The series in Equation (2) converges in when and . Furthermore, the functions defined in (1) and (2) are entire of order and of type for more details, see [3]. The function and its analysis with its generalizations is increasingly becoming a rich research area in mathematics and its related fields. A number of researchers studied and analyzed the function given in (2) (see Wiman [2,4,5]). One can find this function in the study of kinetic equation of fractional order, Lévy flights, random walks, super-diffusive transport as well as in investigations of complex systems. In a similar manner, the advanced studies of these functions reflect and highlight many vital properties of these functions. The function generalizes many functions such as
The interested readers are suggested to go through [6,7,8,9].
Let be the family of all functions g having the form
(3)
and are analytic in and denote the family of univalent functions from . The families of functions which are convex, starlike and close-to-convex of order , respectively, are defined as: andIt is clear that , and Consider the class of all analytic functions in and Baricz [10] introduced the classes
andFor we have the classes of analytic functions and respectively. Also for and we have the classes and .
For the functions given by (1) and given by
then the convolution (Hadamard product) of g and h is defined as:It is clear that the function is not in class . Recently, Bansal and Prajapat [11] considered the normalization of the function given as
In this article, we investigate some geometric properties of function with real parameters and .
We need the following results in our investigations.
([12]). If and
then([13]). Let such that and If satisfies
then is analytic and univalent in .([14]). Let , be analytic in and in addition or then is in class with respect to the function Also if the function which is odd and analytic in and satisfies in addition or then in
([15]). If such that and is analytic in and if is a sequence which is decreasing, i.e., and then
([15]). If and both are non-increasing, then the function g defined by (3) is in
2. Starlikeness, Convexity, Close-to-Convexity
Let and Then,
For the proof of this result, we have to show that
is a decreasing sequence. Consider where ∀ and Now, to show that is decreasing, we prove that .Take
The above expression is non negative ∀ and which shows that is decreasing and convex sequence. Now, from the Lemma 4, we have
which is equivalent to □Let and Then, is starlike in the open unit disc .
To show that is starlike in we prove that and both are non-increasing in view of Lemma 5. Since for the normalized Mittag–Leffler function under the given conditions, consider
for and Now,The above relation is non-negative ∀ and Thus, from Lemma 5, is starlike in . □
Let and Then,
Consider
Here, By taking the same computations as in Theorem 2, we get the proof. □
If and then is in with respect to the function
Set
and we have for all and For the proof of this result, we use Lemma 3. Therefore, we have to show that is decreasing. Now,By restricting parameters, we note that for all Thus, is a decreasing sequence—hence the result. □
If and then is in respect to the function
Set
Here, for all In addition, it is clear that Mainly, we have to show that is decreasing. Now,
By using conditions on parameters, we observe that for all Thus, is a decreasing sequence. By applying Lemma 3, we have the required result. □
Ifand then in .
Let Then, the function p is analytic in with To prove is starlike in , we just prove that in For this, it is enough to show for By using the inequalities
we have(4)
Furthermore, using reverse triangle inequality and the inequality we obtain
(5)
By combining (4) and (5), we get
(6)
Therefore, in if . In other words, we have to show that . The inequality is satisfied for . Hence, is starlike in . □
Recently, Bansal and Prajpat [11] proved that is starlike, if and The above result improves the result in [11].
If and then in .
Let Then, is analytic in with To show that is convex in , it is enough to prove that By using the inequalities
we have(7)
Furthermore, using the inequality then we have
(8)
From (7) and (8), we get
(9)
This implies that in if . To prove our result, we have to show that . The inequality is satisfied for . Hence, is convex in . □
Consider the integral operator , where
Here, We prove that in
Let such that in . If
then in
A calculation gives
Since , then by Schwarz Lemma, triangle inequality and (6), we obtain
By using Lemma 2, in . □
Let and
-
(i)
If then
-
(ii)
If then
-
(iii)
If then
-
(iv)
If then
(i) Using (7) and Lemma 1, we get
where and This shows that(ii) To prove we have to show that where By using triangle inequality with
(see [16]), where is the largest root of the equation we have This implies that for(iii) We use the inequality to show the starlikeness of order for the function By using (4) and (5), we have
This implies that
This completes the proof.
(iv) We use the inequality to show that By using (7) and (8), we have
This implies that
hence the result. □Substituting in Theorem 9, we obtained the following results.
Let .
-
(i)
If then
-
(ii)
If then
-
(iii)
If then
-
(iv)
If then
It is clear that when and when It concludes that our results improve the results of ([17], corollary 2.1).
3. Hardy Space of Mittag–Leffler Function
Consider the class of analytic functions in and denote the space bounded functions on . Let , set
If is bounded for then . It is clear that
For some details, see [18]. It is also known [18] that, if in , then
Hardy spaces of certain special functions are studied in [10,19,20].
([21]). where and The value γ can not be improved.
([22]). For and we have or equivalently
([23]). If the function g, convex of order μ, where , is not of the form
for , and then the following statements are true:- (i)
There existsuch that
- (ii)
Ifthen there existssuch that
- (iii)
Ifthen
Let,
- (i)
Ifthen
- (ii)
Ifthen
By using the definition of the hypergeometric function
we have for and for real On the other hand,Therefore, the function is not of the form of and We know that, by part (iv) of Theorem 9, Therefore, by using Lemma 8, we have the required result. □
Let and Then, convolution is in
Let Then, Using the Corollary 1 part ii, we have As ; therefore, by using Lemma 6 Now, the function is complete; therefore, is complete. This implies that is bounded. Thus, we have the required result. □
Let and If then where
Let Then, it is clear that Using Theorem 9 part (ii), we have As , therefore, by using Lemma 6 and the fact that we have where Consequently, □
Let and If , then
Let and If , then
4. Applications
Now, we present some applications of the above theorems. It is clear that
From Theorem 9, we get the following:
If where then
If where then
If where then
If where then
Let , where If , then
Let , where If , then
Let , where If , then
5. Conclusions
In this paper, we have studied certain geometric properties of Mittag-Leffler functions such as starlikeness, convexity and close-to-convexity. We have also found the Hardy spaces of Mittag-Leffler functions. Further, we have improved some results in the literature.
Author Contributions
Conceptualization, S.N. and M.R.; Formal analysis, S.N. and M.R.; Funding acquisition, J.L.L.; Investigation, S.N.; Methodology, S.N. and M.R.; Supervision, M.R.; Validation, M.A.; Visualization, M.A.;Writing—original draft, S.N.; Writing—review and editing, J.L.L.
Funding
The work presented here is supported by the Natural Science Foundation of Jiangsu Province under Grant No. BK20151304 and the National Natural Science Foundation of China under Grant No. 11571299.
Acknowledgments
The authors are grateful to the referees for their valuable comments and suggestions which improve the presentation of paper.
Conflicts of Interest
The authors declare no conflict of interest.
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© 2019 by the authors.
Abstract
The aim of this paper is to investigate certain properties such as convexity of order
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Details
1 Department of Mathematics, Government College University, Faisalabad 38000, Pakistan
2 Department of Mathematics, Yangzhou University, Yangzhou 225002, China
3 Department of Mathematics, Abdul Wali Khan University Mardan, Mardan 23200, Pakistan