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Research article

Applications of a differential operator to a class of harmonic mappings defined by Mittag-leffer functions

  • Received: 02 April 2020 Accepted: 26 August 2020 Published: 02 September 2020
  • MSC : 30C45, 30C50

  • Utilizing the concepts of Harmonic analysis and Mittag-Leffler functions we introduce a new subclass of harmonic mappings involving differential operator in domain of Janowski functions. Moreover, we investigate analytic criteria, necessary and sufficient conditions, topological properties, extreme points, radii problems and some applications of this work for the class of functions defined by this operator.

    Citation: Muhammad Ghaffar Khan, Bakhtiar Ahmad, Thabet Abdeljawad. Applications of a differential operator to a class of harmonic mappings defined by Mittag-leffer functions[J]. AIMS Mathematics, 2020, 5(6): 6782-6799. doi: 10.3934/math.2020436

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  • Utilizing the concepts of Harmonic analysis and Mittag-Leffler functions we introduce a new subclass of harmonic mappings involving differential operator in domain of Janowski functions. Moreover, we investigate analytic criteria, necessary and sufficient conditions, topological properties, extreme points, radii problems and some applications of this work for the class of functions defined by this operator.


    The study of analytic functions has been the core interest of various prominent researchers in the last decade. Much emphasis has been on the aspect of introduction of various concepts in this field. Uralegaddi [1], in 1994, introduced the subclasses of starlike, convex and close-to-convex functions with positive coefficients and opened a new side of Geometric Function Theory. Motivated by his work Dixit and Chandra [2] introduced new subclass of analytic functions with positive coefficients. Continuing the trend Dixit et al. [3], Porwal and Dixit [4] and Porwal et al. [5] made a substantial amount of important theory which illuminated various new directions of this field. One such area is Harmonic Analysis which has vastly influenced and nurtured the branch of Geometric Function Theory. Dixit and Porwal [6] defined and investigated the class of harmonic univalent functions with positive coefficients. With the introduction of this work many mathematicians generalized various important results with the help of some operators, the work of Pathak et al. [7], Porwal and Aouf [8] and Porwal et al. [9] are worth mentioning here. More recently new subclasses of harmonic starlike and convex functions are introduced and studied by Porwal and Dixit [10], see also [5].

    Recently attention has been drawn to Mittag-Leffer functions as these functions can be widely applied across the fields of engineering, chemical, biological, physical sciences as will as in various other applied sciences. Various factors in applying such functions are evident within chaotic, stochastic, dynamic systems, fractional differential equations and distribution of statistics. The geometric characteristics such as convexity, close-to-convexity and starlikeness of the functions investigated here has been broadly examined by many authors. Direct applications of these functions can be seen in a number of fractional calculus tools which includes significant work by [11,12,13,14,15,16,17,18,19,20].

    Before we go into details about our new work we give some basics which will be helpful in understanding the concepts of this research.

    A real-valued function u(x,y) is said to be harmonic in a domain DC if it has continuous second partial derivative and satisfy the Laplace's equation

    2ux2+2uy2=0,

    and complex-valued function f=u+iv is said to be harmonic in a domain D if and only if u and v are both real harmonic functions in domain D. Every complex-valued harmonic function f which is harmonic in D, containing the origin, can be represented in the canonical form as

    f=h(z)+¯g(z), (1.1)

    where h and g are analytic functions in D with g(0)=0.Then functions h and g are known as analytic and co-analytic parts of f respectively. The Jacobian of f=u+iv is given by

    Jf(z)=|uxvxuyvy|=uxvyvxuy ,

    which can be represented in terms of derivatives with respect to z and ¯z as

    Jf(z)=|fz|2|f¯z|2=|h(z)|2|g(z)|2 (zD).

    It can be noted that if f is analytic in D, then f¯z=0 and fz(z)=f(z). A well- known result for analytic functions state that an analytic function f is locally univalent at a point z0 if and only if Jf(z)0 in D (see for example [21]). In [22], Lewy proved the converse of this theorem which is also true for harmonic mappings. Therefore, f is sense-preserving and locally univalent if and only if

    |h(z)|>|g(z)| (zD). (1.2)

    Let H denote the class of functions f which are harmonic in the unit disc A:=A(1), where A(r):={zC:|z|<r}. Also, let H0 denote the class of functions fH which satisfy the normalization conditions

    f(0)=f¯z(0)=f(0)1=0.

    Therefore the analytic functions h and g given by (1.1) can be written in the form

    h(z)=z+n=2anzn, g(z)=n=2bnzn (zA),

    and

    f(z)=z+n=2(anzn+¯bnzn) (zA). (1.3)

    Let

    SH:={fH0:f is univalent and sense-preserving in A}.

    It is clear that SH reduces to the class S, and by A whenever the co-analytic part of f vanishes, i.e., g(z)=0 in A. Clunie and Sheil-Small [23] and Sheil-Small [24] studied SH together with some of its geometric subclasses. We say that a function fH0 is said to be harmonic starlike in A if it satisfy

    ReDHf(z)f(z)>0,

    where

    DHf(z):=h(z)¯g(z) (zA).

    A function f(z) is subordinated to a function g(z) denoted by f(z)g(z), if there is complex-valued function w(z) with |w(z)|1 and g(0)=0 such that

    f(z)=g(w(z)) (zA).

    Also, if g(z) is univalent in A, we have equivalence condition

    f(z)g(z),  zA    f(0)=g(0)  and  f(A)g(A).

    Convolution or Hadamard product of two function f1 and f2 is denoted by f1 f2 and is defined by

    (f1f2)(z)=z+n=2(a1a2zn+¯b1b2zn)  (zA). (1.4)

    In 1973, Janowski [25] introduced the idea of circular domain by introducing Janowski functions as;

    A function k(z), analytic in A with k(0)=1, is said to be in class T[A,B] if for 1B<A1

    k(z)1+Az1+Bz.

    Janowski showed that the function k maps A onto the domain Δ(A,B) with centre on real axis and D1=1A1B and D2=1+A1+B are diameter end points with 0<D1<1<D2.

    The Mittag-Leffer function is defined as

    Eα(z)=n=0znΓ(αn+1). (1.5)

    The initial two parametric generalizations for the function shown in (1.5) were given by Wiman [26,27]. It is defined in the following way

    Eα,β(z)=n=0znΓ(αn+β),

    where α,βC, Re(α)>0, Re(β)>0 and Γ(z) is gamma function.

    Now the function Qα,β is defined by

    Qα,β(z)=zΓ(β)Eα,β(z)=z+n=2Γ(β)Γ(α(n1)+β)zn.

    Using the function Qα,β Elhaddad et al. [28] defined the differential operator for the class of analytic functions as Dmδ(α,β):AA as illustrated below :

    Dmδ(α,β)f(z)=f(z)Qα,β(z),
    Dmδ(α,β)f(z)=z+n=2[1+(n1)δ]mΓ(β)Γ(α(n1)+β)anzn, (1.6)

    where m=N0={0,1,2,...}, δ>0.

    Where the operator Dmδ(α,β) for a function fH given by (1.1) can be defined as below:

    Dmδ(α,β)f(z)=Dmδ(α,β)h(z)+¯Dmδ(α,β)g(z) (zA),

    where

    Dmδ(α,β)h(z)=z+n=2[1+(n1)δ]mΓ(β)Γ(α(n1)+β)anzn,Dmδ(α,β)g(z)=z+n=2[1+(n1)δ]mΓ(β)Γ(α(n1)+β)bnzn,

    for mN0.

    Motivated by [29,30] and using the operator Dmδ(α,β)f(z), we introduced the class of harmonic univalent functions as:

    Definition Let BA<B1, 0a<1  and Sα,βH(m,δ,A,B) denote the class of functions fSH such that

    DH(Dmδ(α,β)f(z))Dmδ(α,β)f(z)1+Az1+Bz, (1.7)

    with

    DH(Dmδ(α,β)f(z)):=DH(Dmδ(α,β)h(z))¯DH(Dmδ(α,β)g(z)).

    Note that,

    1. S0,1H(0,δ,A,B)=SH(A,B), which was studied by Deziok [29].

    2. S0,1H(0,δ,2a1,1)=SH(a), defined by Jahangiri in [31]

    3. S0,1H(1,1,2a1,1)=ScH(a), introduced by Jahangiri, see [32] for details.

    Let VH0, A0=A{0}. Using Ruscheweyh's approach in [33] we define the dual set of V by

    V:={fH0:ΛgV(fg)0 (zA0)}

    In this section we prove some important results beginning with necessary and sufficient condition. Then some inequality regarding the coefficients of the functions in their series form are evaluated along with examples for justifications.

    Let fH0 and is given by (1.3) is in the class Sα,βH(m,δ,A,B) if and only if

    Sα,βH(m,δ,A,B)={Dmδ(α,β)φξ(z); |ξ|=1} ,

    where

    φξ(z)=z1+Bξ(1+Aξ)(1z)(1z)2¯z1+Bξ(1+Aξ)(1¯z)(1¯z)2 (zD).

    Proof. Let fH0, then fSα,βH(m,δ,A,B) if and only if the following holds

    DH(Dmδ(α,β)f(z))Dmδ(α,β)f(z)1+Aξ1+Bξ (ξC, |ξ|=1).

    Now as

    DH(Dmδ(α,β)h(z))=Dmδ(α,β)h(z)z(1z)2

    and

    Dmδ(α,β)h(z)=Dmδ(α,β)h(z)z1z,

    thus

    (1+Bξ)DH(Dmδ(α,β)f(z))(1+Aξ)Dmδ(α,β)f(z)=(1+Bξ)DH(Dmδ(α,β)h(z))(1+Aξ)Dmδ(α,β)h(z)[(1+Bξ)DH(¯Dmδ(α,β)g(z))+(1+Aξ)¯Dmδ(α,β)g(z)]=Dmδ(α,β)h(z)((1+Bξ)z(1z)2(1+Aξ)z1z)¯Dmδ(α,β)g(z)((1+Bξ)¯z(1¯z)2+(1+Aξ)¯z1¯z)=f(z)Dmδ(α,β)φξ(z)0 (zA0, |ξ|=1).

    Thus fSα,βH(m,δ,A,B) if and only if f(z)Dmδ(α,β)φξ(z)0 for zA0, |ξ|=1 i.e. Sα,βH(m,δ,A,B)={Dmδ(α,β)φξ(z); |ξ|=1}.

    A sufficient coefficient bound for the class Sα,βH(m,δ,A,B) is provided in the following.

    Let fH0 be of the form (1.3) and satisfies the condition

    n=2(λn|an|+σn|bn|)BA, (2.1)

    with

    λn=|[1+(n1)δ]mΓ(β)Γ(α(n1)+β)|[(1+B)n(1+A)], (2.2)
    σn=|[1+(n1)δ]mΓ(β)Γ(α(n1)+β)|[(1+B)n+(1+A)], (2.3)

    then fSα,βH(m,δ,A,B).

    Proof. Obviously the theorem is true for f(z)=z. Suppose fH0 given by (1.3) and let there exist n2 such that an0 or bn0. Since

    λnBAn,  σnBAn,  n=2,3,...,

    by (2.1) we have

    n=2(n |an|+n |bn|)1 (2.4)

    and

    |h(z)||g(z)|1n=2n |an||z|nn=2n |bn||z|n1|z|n=2(n |an|+n |bn|)1|z|BAn=2(λn|an|+σn|an|)1|z|>0 (zA).

    Therefore|h(z)|>|g(z)| which shows that f is locally univalent and sense-preserving in A. Moreover ifz1,z2A and z1z2 then

    |zn1zn2z1z2|=|nk=1zk11znk2|nk=1|zk11||znk2|<n  (n=2,3,..).

    Hence by (2.4) we have

    | f(z1)f(z2)||h(z1)h(z2)||g(z1)g(z2)||z1z2n=2an(zn1zn2)||n=2¯bn(zn1zn2)||z1z2|n=2|an||zn1zn2|n=2|bn||zn1zn2|=|z1z2|(1n=2|an||zn1zn2z1z2|n=2|bn||zn1zn2z1z2|)>|z1z2|(1n=2n |an|n=2n |bn|)0.

    This shows that f is univalent, i.e. fSH. Therefore fSα,βH(m,δ,A,B) if and only if there exists a complex-valued function ω, ω(0)=0, |ω(z)|<1 (zA), such that

    DH(Dmδ(α,β)f(z))Dmδ(α,β)f(z)=1+Aω(z)1+Bω(z)  (zA),

    or equivalently

    |DH(Dmδ(α,β)f(z))Dmδ(α,β)f(z)BDH(Dmδ(α,β)f(z))ADmδ(α,β)f(z)|<1  (zA). (2.5)

    Thus, it is sufficient to prove that

    |DH(Dmδ(α,β)f(z))Dmδ(α,β)f(z)||BDH(Dmδ(α,β)f(z))ADmδ(α,β)f(z)|<0,

    where zA{0}, now by putting |z|=r,  r(0,1) we get

    |DH(Dmδ(α,β)f(z))Dmδ(α,β)f(z)||BDH(Dmδ(α,β)f(z))ADmδ(α,β)f(z)|=|n=2[1+(n1)δ]mΓ(β)Γ(α(n1)+β)(n1)anznn=2[1+(n1)δ]mΓ(β)Γ(α(n1)+β)(n+1)¯bnzn||(BA)z+n=2[1+(n1)δ]mΓ(β)Γ(α(n1)+β)(BnA)anzn[1+(n1)δ]mΓ(β)Γ(α(n1)+β)(Bn+A)¯bnzn|,n=2|[1+(n1)δ]mΓ(β)Γ(α(n1)+β)|(n1)|an|rn+n=2|[1+(n1)δ]mΓ(β)Γ(α(n1)+β)|(n+1)|bn|rn(BA)r+n=2|[1+(n1)δ]mΓ(β)Γ(α(n1)+β)|(BnA)|an|rn                 +n=2|[1+(n1)δ]mΓ(β)Γ(α(n1)+β)|(Bn+A)|bn|rnr{n=2(λn|an|+σn|bn|)rn(BA)}<0,

    hence fSα,βH(m,δ,A,B).

    For function

    f(z)=z+n=2pnBAλnzn+n=2qnBAσn¯zn (zA),

    such that n=2(|pn|+|qn|)=1, we have

    n=2(λn|an|+σn|bn|)=n=2(|pn|(BA)+|qn|(BA))=(BA)n=2(|pn|+|qn|)=(BA).

    Thus fSα,βH(m,δ,A,B) and above inequality (2.1) is sharp for this function.

    Motivated from Silverman [34], we introduce the class τ for functions fH0 of the form (1.3) such that an=|an|, bn=|bn| (n=2,3,...), i.e.

    f(z)=h(z)+¯g(z), h(z)=zn=2|an|zn, g(z)=n=2|bn|¯zn (zA). (2.6)

    Further, let us define

    Sα,βτ(m,δ,A,B)=τSα,βH(m,δ,A,B).

    Where α=0, β=1 and m=0 the class is studied by Dziok see [29].

    Let fτ and of the form (2.6). Then f Sα,βτ(m,δ,A,B) if and only if condition (2.1) holds true.

    Proof. In Theorem 2.2 we need only to show that each function f Sα,βτ(m,δ,A,B) satisfies coefficient inequality (2.1). If f Sα,βτ(m,δ,A,B) then it is of the form (2.6) and satisfies (2.5) or equivalently

    |n=2[1+(n1)δ]mΓ(β)Γ(α(n1)+β)(n1)anznn=2[1+(n1)δ]mΓ(β)Γ(α(n1)+β)(n+1)¯bnzn(BA)zn=2[1+(n1)δ]mΓ(β)Γ(α(n1)+β)(BnA)anznn=2[1+(n1)δ]mΓ(β)Γ(α(n1)+β)(Bn+A)¯bnzn|<1 ,

    where zA, therefore by putting z=r , r[0,1), we get

    n=2|[1+(n1)δ]mΓ(β)Γ(α(n1)+β)|[(n1)|an|+(n+1)|bn|]rn1(BA)+n=2|[1+(n1)δ]mΓ(β)Γ(α(n1)+β)|{(BnA)|an|+(Bn+A)|bn|}<1. (2.7)

    It is clear that the denominator of the left hand side cannot vanishes for r(0,1). Moreover, it is positive for r=0, and in consequence for r(0,1). Thus, by (2.7) we have

    n=2(λn|an|+σn|bn|)rn1BA  r[0,1). (2.8)

    The sequence of partial sums {Sn} associated with the series n=2(λn|an|+σn|bn|) is a non-decreasing sequence. Moreover, by (2.8) it is bounded by BA. Hence, the sequence {Sn} is convergent and

    n=2(λn|an|+σn|bn|)rn1=limnSnBA,

    which yields assertion (2.1).

    For function

    f(z)=zn=2cnBAλnzn+n=2dnBAσn¯zn (zA),

    such that n=2(|cn|+|dn|)=1, we have

    n=2(λn|an|+σn|bn|)=n=2(|cn|(BA)+|dn|(BA))=(BA)n=2(|cn|+|dn|)=(BA).

    Thus fSα,βτ(m,δ,A,B).

    we consider the usual topology on H in which a sequence {fn} in H converges to f if and only if it converges to f uniformly on each compact subset of A. The metric induces the usual topology on H. It is to verify that the obtained topological space is complete.

    Let F be a subclass of the class H. A function fF is called an extreme point of F if the condition

    f=γf1+(1γ)f2    (f1,f2F, 0<γ<1)

    implies f1=f2=f. We shall use the notation EF to denote the set of all extreme points of F. It is clear that EFF.

    We say that F is locally uniformly bounded if for each r, 0<r<1, there is a real constant M=M(r) so that

    |f(z)|M  (fF|z|r).

    We say that a class F is convex if

    γf+(1γ)gF  (f,gF, 0γ1).

    Moreover, we define the closed convex hull of F as the intersection of all closed convex subsets of H that contain F. We denote the closed convex hull of F by ¯coF.

    A real-valued function J:HR is called convex on a convex class FH if

    J(γf+(1γ)g)γJ(f)+(1γ)J(g)  (f,gF, 0γ1).

    The Krein-Milman theorem (see [35]) is fundamental in the theory of extreme points. In particular, it implies the following lemma.

    Let F be a non-empty convex compact subclass of the class H and let J:HR be a real-valued, continuous and convex function on F. Then

    max{J(f):fF}=max{J(f):fEF}.

    A class FH is compact if and only if F is closed and locally uniformly bounded.

    Since H is complete metric space, Montel's theorem (see [36]) implies the following lemma.

    Let F be a non-empty compact subclass of the class H, then EF is non-empty and ¯coEF=¯coF.

    The class Sα,βτ(m,δ,A,B) is a convex and compact subset of H.

    Proof. Let flSα,βτ(m,δ,A,B) be a functions of the form

    fl(z)=zn=2(|al,n|zn|bl,n|¯zn) (zA, lN={1,2,3,...}), (3.1)

    and 0γ1. Since

    γf1(z)+(1γ)f2(z)=                   
    zn=2{(γ|a1,n|+(1γ)|a2,n|)zn+(γ|b1,n|+(1γ)|b2,n|)}¯zn

    and by Theorem 2.4, we have

    n=2{αn(γ|a1,n|+(1γ)|a2,n|)zn+βn(γ|b1,n|+(1γ)|b2,n|)}=γn=2{αn|a1,n|+βn|b1,n|}+(1γ)n=2{αn|a2,n|+βn|b2,n|}γ(BA)+(1γ)(BA)=BA,

    the function Ψ=γf1+(1γ)f2Sα,βτ(m,δ,A,B). Hence, the class is convex. Furthermore, for fSα,βτ(m,δ,A,B), |z|r r(0,1), we have

    |f(z)|r+n=2(|an|+|bn|)rnr+n=2(αn|an|+βn|bn|)r+(BA). (3.2)

    Thus, we conclude that the class Sα,βτ(m,δ,A,B) is locally uniformly bounded. By Lemma 3.2, we need only to show that it is closed, i.e. if flf, then fSα,βτ(m,δ,A,B). Let fl and f be given by (3.1) and (2.6), respectively. Using Theorem 2.4, we have

    n=2(αn|ai,n|+βn|bi,n|)BA  (iN). (3.3)

    Since fif, we conclude that  |ai,n||an| and |bi,n||bn| as i (nN). The sequence of partial sums {Sn} associated with the series n=2(αn|ai,n|+βn|bi,n|) is non-decreasing sequence. Moreover, by (3.3) it is bounded by BA. Therefore, the sequence {Sn} is convergent and

    n=2(αn|ai,n|+βn|bi,n|)=limn{Sn}BA.

    This gives condition (2.1) and in consequence, fSα,βτ(m,δ,A,B), which complete the proof.

    We have

    ESα,βτ(m,δ,A,B)={hn:nN}{gn:n{2,3,...}},

    where

    h1(z)=z, hn(z)=z BAλnzn, gn(z)=z +BAσn¯zn (n=2,3,..., zA) (3.4)

    Proof. Suppose that 0<γ<1 and

    gn(z)=γf1+(1γ)f2,

    where f1, f2Sα,βτ(m,δ,A,B) are functions of the form (3.1). Then, by (2.1) we have

    |b1,n|=|b2,n|=BAσn,

    and, in consequence, a1,i=a2,i=0 for i{2,3,...} and b1,i=b2,i=0 for i{2,3,...}{n}. It follows that gn=f1=f2, and consequently gnESα,βτ(m,δ,A,B). Similarly, we verify that the functions hn of the form (3.4) are extreme points of the class Sα,βτ(m,δ,A,B). Now, suppose that fESα,βτ(m,δ,A,B) and f is not of the form (3.4). Then there exists i{2,3,...} such that

     0<|ai|<BAλi  or 0<|bi|<BAσi.

    If 0<|ai|<BAλi, then putting

    γ=|ai|λiBA, Φ=11γ(fγhi),

    we have that 0<γ<1, hi, Φ Sα,βτ(m,δ,A,B), hiΦ and

     f=γhi+(1γ)Φ.

    Thus, fESα,βτ(m,δ,A,B). Similarly, if 0<|bi|<BAσi, then putting

    γ=|bi|σiBA, Ψ=11γ(fγgi),

    we have that 0<γ<1, gi, ΦSα,βτ(m,δ,A,B), giΨ and

    f=γgi+(1γ)Ψ.

    It follows that fESα,βτ(m,δ,A,B), and this completes the proof.

    A function fH0 is said to be starlike of order α in A(r) if

    t(argf(ρeit))>α, 0t2π, 0<ρ<r<1. (4.1)

    Also, A function fH0 is said to be convex of order α in A(r) if

    t(t(argf(ρeit)))>α,0t2π,0<ρ<r<1.

    It easy to verify that for function fτ the condition (4.1) is equivalent to the following

    ReDHf(z)f(z)>α (zA(r)),

    or equivalently

    |DHf(z)(1+α)f(z)DHf(z)+(1+α)f(z)|<1 (zA(r)). (4.2)

    Let B be a subclass of the class H0. We define the radius of starlikeness and convexity

    Rα(B)=inffB(sup{r(0,1]:f is starlike of order α in A(r)}),Rcα(B)=inffB(sup{r(0,1]:f is convex of order α in A(r)}).

    In simple word these show the subregion of the open unit disc where the functions would behave starlike and convex of order α.

    The radii of starlikeness of order α for the class Sα,βτ(m,δ,A,B) is given by

    Rα(Sα,βτ(m,δ,A,B))=infn2(1αBAmin{λnnα,σnn+α})1n1, (4.3)

    where λn and σn are define in (2.2) and (2.3) respectively.

    Proof. Let fSα,βτ(m,δ,A,B) be of the form (2.6). Then, for |z|=r<1 we have

    |DHf(z)(1+α)f(z)DHf(z)+(1+α)f(z)|=|αz+n=2((n1α)|an|zn(n+1+α)|bn|¯zn)(2α)z+n=2((n+1α)|an|zn(n1+α)|bn|¯zn)|α+n=2((n1α)|an|(n+1+α)|bn|)rn1(2α)n=2((n+1α)|an|(n1+α)|bn|)rn1.

    Thus the condition (4.2) is true if and only if

    n=2(nα1α|an|+n+α1α|bn|)rn11. (4.4)

    By Theorem 2.2, we have

    n=2(λnBA|an|+σnBA|bn|)1, (4.5)

    where λn and σn are defined by (2.2) and (2.3) respectively. Thus the conditions (4.4) is true if

    nα1αrn1λnBA,n+α1αrn1σnBA(n=2,3,...),

    i.e.,

    r(1αBAmin{λnnα,σnn+α})1n1 (n=2,3,...).

    It follows that the function f is starlike of order α in the disc A(r), where r

    r:=inf(1αBAmin{λnnα,σnn+α})1n1.

    The functions hn and gn are define by (3.4) realize equality in (4.5), and the radius r cannot be larger, thus we have (4.3).

    The following theorem may be proved in much same fashion as Theorem 4.1..

    The radii of convexity of order α for the class Sα,βτ(m,δ,A,B) is given by

    Rcα(Sα,βτ(m,δ,A,B))=infn2(1αBAmin{λnnα,σnn+α})1n1,

    where λn and σn are define in (2.2) and (2.3) respectively.

    In this section we give some applications of the work discussed in this article in the form of some results and examples. It is clear that if the class

    F={fnH:nN}

    is locally uniformly bounded, then

    ¯coF={n=1γnfn:n=2γn=1,γn0 (nN)} (5.1)
    Sα,βτ(m,δ,A,B)={n=2(γnhn+δngn):n=2(γn+δn)=1,δ1=0, γn,δn0 (nN)}, (5.2)

    where hn and gn are defined by Eq (3.4).

    Proof. By Theorem 3.4 and Lemma 3.3 we have

    Sα,βτ(m,δ,A,B)=¯coSα,βτ(m,δ,A,B)=¯coESα,βτ(m,δ,A,B).

    Thus, by Theorem 3.5 and by (5.1) we have Eq (5.2).

    We observe, that for each nN, zA, the following real-valued functionals are continuous and convex on H:

    J(f)=|an|, J(f)=|bn|, J(f)=|f(z)|, J(f)=|DHf(z)| (fH),

    and

    J(f)=(12π2π0|f(reiθ)|γdθ)1γ  (fH,γ1,0<r<1).

    Therefore, using Lemma 3.1 and Theorem 3.5 we have the following corollaries.

    Let fSα,βτ(m,δ,A,B) be a function of the form (2.6). Then

    |an|BAλn, |bn|BAσn (n=2,3,...). (5.3)

    where λn and σn are defined by (2.2) and (2.3) respectively. The result is sharp. The function hn and gn of the form (3.4) are extremal functions.

    Proof. Since for the extremal functions hn and gn we have |an|=BAλn and |bn|=BAσn. Thus, by Lemma 3.1 we have Eq (5.3).

    Since BA+2λ2>BAλ2 the polynomial

    k(z)=zBA+2λ2z2 (zA),

    by Corollary 5.2, clearly k(z) does not belong to Sα,βτ(m,δ,A,B).

    Let fSα,βτ(m,δ,A,B), |z|=r<1. Then

    r|Γ(α+β)[1+δ]mΓ(β)|BA(1+2BA)r2|f(z)|r+|Γ(α+β)[1+δ]mΓ(β)|BA(1+2BA)r2,r|Γ(α+β)[1+δ]mΓ(β)|2(BA)(1+2BA)r2|DHf(z)|r+|Γ(α+β)[1+δ]mΓ(β)|2(BA)(1+2BA)r2.

    Due to Littlewood [37] we consider the integral means inequalities for functions from the class Sα,βτ(m,δ,A,B).

    Let f,gA. If fg, then

    2π0|f(reiθ)|γdθ2π0|g(reiθ)|γdθ .

    Let 0<r<1, γ>0. Then

    12π2π0|hn(reiθ)|γdθ12π2π0|h2(reiθ)|γdθ  (n=2,3,...), (5.4)

    and

    12π2π0|gn(reiθ)|γdθ12π2π0|h2(reiθ)|γdθ  (n=2,3,...), (5.5)

    where hn and gnis defined by Eq (3.4).

    Proof. Let hn and gn are define by Eq (3.4) and let ~gn(z)=z+BAσnzn (n=2,3,...). Since hnzh2z and ~gnzh2z, by Lemma 5.5 we have

    2π0|hn(reiθ)|γdθ2π0|h2(reiθ)|γdθ,

    and

    2π0|gn(reiθ)|γdθ=2π0|~gn(reiθ)|γdθ2π0|h2(reiθ)|γdθ,

    which complete the proof.

    If fSα,βτ(m,δ,A,B) then

    12π2π0|f(reiθ)|γdθ12π2π0|h2(reiθ)|γdθ,

    and

    12π2π0|DHf(reiθ)|γdθ12π2π0|DHh2(reiθ)|γdθ,

    where γ1, 0<r<1 and h2 is the function defined by Eq (3.4).

    With the use of Mittag-Leffer functions, we introduced a new subclass of harmonic mappings in Janowski domain. We studied some useful results, like necessary and sufficient conditions, coefficient inequality, topological properties, radii problems, distortion bounds and integral mean of inequality for newly defined classes of functions. It can be seen that our defined class not only generalizes various well known classes and their respective results but also give new direction to this field by the introduction of Mittag-Leffer functions here. Further using the concepts of Mittag-Leffer functions these problems can be studied for classes of meromorphic harmonic functions, Bazilevi'c harmonic functions and for p-valent harmonic functions as well.

    The authors declare that they have no competing interests.



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