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Based on a family of bi-univalent functions introduced through the Faber polynomial expansions and Noor integral operator

  • In this study, by using q-analogue of Noor integral operator, we present an analytic and bi-univalent functions family in D. We also derive upper coefficient bounds and some important inequalities for the functions in this family by using the Faber polynomial expansions. Furthermore, some relevant corollaries are also presented.

    Citation: F. Müge Sakar, Arzu Akgül. Based on a family of bi-univalent functions introduced through the Faber polynomial expansions and Noor integral operator[J]. AIMS Mathematics, 2022, 7(4): 5146-5155. doi: 10.3934/math.2022287

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  • In this study, by using q-analogue of Noor integral operator, we present an analytic and bi-univalent functions family in D. We also derive upper coefficient bounds and some important inequalities for the functions in this family by using the Faber polynomial expansions. Furthermore, some relevant corollaries are also presented.



    Conformal mapping is used in electromagnetic theory as well as in heat transfer theory. Univalent functions have wide application in heat transfer problems (see [16]). Special functions contain a very old branch of mathematics. In addition, in recent years, special functions and inequalities are widely used for solving some problems in physics, integer-order differential equations and systems, electromagnetizm, heat-transfer problems, mathematical models, etc [24]. Specially harmonic, analytical functions and inequalities of coefficients are widely used in thermodynamics, electricity and magnetism and quantum physics. In electricity, current and impedance equations can be expressed in a complex plane, and basic electrical relations become complex functions. However, in this study, we consider only upper coefficient bounds and some important inequalities for analytic and bi-univalent functions family by using special functions.

    Let's denote by C which is the complex plane in the open unit disk D={z:zCand|z|<1}. Additionaly, A denotes the family of functions s(z) which are analytic in the open unit disk and normalized by s(0)=s(0)1=0 and having the style:

    s(z)=z+k=2akzk. (1.1)

    Let S be a subfamily of A which is univalent in D (for details, see [11]). Furthermore, P be the family of functions, formed:

    φ(z)=1+k=1φkzk(zD)

    D and hold the necessity (φ(z))>0 in D. By the Carathéodory's Lemma (e.g., see [11]), we get |φk|2.

    In accordance with the Koebe Theorem (e.g., see [11]), each univalent function s(z)A has an inverse s1 fulfilling

    s1(s(z))=z(zD)

    and

    s(s1(w))=w(|w|<r0(s)r0(s)14).

    Actually, the inverse function s1 is denoted by

    r(w)=s1(w)=wa2w2+(2a22a3)w3(5a325a2a3+a4)w4+. (1.2)

    If both s(z) and s1(z) are univalent, we can say that, sA is be bi-univalent in D. All families of bi-univalent functions in D with Taylor-Maclaurin series expansion (1.1) are presented by Σ.

    For both of some knowledges and different examples for functions belong to Σ, see the following references [9,17,18,22,23,25]. Also, see references by Ali et al. [5], Jahangiri and Hamidi [15], and other studies such as [6,7,10,13,21].

    Definition 1. For analytic functions s and r,s is subordinate to r, presented by

    s(z)r(z), (1.3)

    if there is an analytic function w such that

    w(0)=0 , |w(z)|<1 ands(z)=r(w(z)).

    The following definition gives us the knowledge about fractional q-calculus operators (see, [22]).

    Definition 2. [22] For q(0,1), the q-derivative of sA is given by

    qs(z)=s(qz)s(z)(q1)z,z0 (1.4)

    and

    qs(0)=s(0).

    Thus we have

    qs(z)=1+k=2[k,q]akzk1 (1.5)

    where [k,q] is presented by

    [k,q]=1qk1q,   [0,q]=0 (1.6)

    and define the q-fractional by

    [k,q]!={kn=1[n,q],kN1,k=0. (1.7)

    Furthermore, Pochhammer symbol which is qgeneralized for p0 is denoted by

    [p,q]k={kn=1[p+n1,q],kN1,k=0. (1.8)

    In addition, as q1,[k,q]k, if we select r(z)=zk, then we obtain

    qr(z)=qzk=[k,q]zk1=r(z),

    where r is the ordinary derivative.

    Recently, F1q,μ+1(z), given with the following relation, was defined by Arif et al. (see[8])

    F1q,μ+1(z)Fq,μ+1(z)=zqs(z),  (μ>1) (1.9)

    where

    Fq,μ+1(z)=z+k=2[μ+1,q]k1[k1,q]!zk,  zD. (1.10)

    Due to the fact that series given in (1.10) is convergent absolutely in zD, by taking advantage of the characterization of q -derivative via convolution, one can define the integral operator ζμq:DD by

    ζμqs(z)=F1q,μ+1(z)s(z)=z+k=2ϕk1akzk,  (zD) (1.11)

    where

    ϕk1=[k,q]![μ+1,q]k1. (1.12)

    We note that

    ζ0qs(z)=zqs(z),ζqs(z)=s(z) (1.13)

    and

    limq1ζμqs(z)=z+k=2k!(μ+1)k1akzk. (1.14)

    Equation (1.14) means that the operator denoted by (1.11) reduces to the known Noor integral operator by getting q1, which is presented in (see[19,20]). For further informations on the q-analogue of differential-integral operators, see the study of Aldweby and Darus (see[4]).

    This work was motivated by Akgül and Sakar's study [3]. The basic purpose of this study is to give a new subfamily, which is in Σ and provide general coefficient bound |an| by using Faber polynomial technics for this subfamily. Additionaly, we derive bounds of the |a2| and |a3| which are the first two coefficients of this subfamily.

    In this part, firstly we will introduce the class Wμ,qΣ(α,τ;φ) and then give the knowledgements about Faber polynomial expansions.

    Definition 3. A function sΣ is known in the class Wμ,qΣ(α,τ;φ) if the requirements given below hold:

    1+1τ[(1α)ζμqs(z)z+αq(ζμqs(z))1]φ(z)(zD), (2.1)

    and

    1+1τ[(1α)ζμqr(w)w+αq(ζμqr(w))1]φ(w)(wD) (2.2)

    where (μ>1,0<q<1, τ>0,α0) and s=r1(w) is given by (1.2).

    It is clear from Definition 3 that upon setting q1, for τ=1, α=1 and μ=1, one can easily see that sΣ is in  

    W1Σ(1,1;φ)=Hσ(φ)

    if the conditions given below hold true:

    s(z)φ(z)(zD),

    and

    r(w)φ(w)(wD),

    where r=s1 is given by (1.2). The class Hσ(φ) was investigated by Ali et al. [5].

    The Faber polynomials act effective role in several fields of mathematical sciences, specially, in the Theory of Geometric Function [12]. Also, Grunsky [14] gave some sufficient conditions for the univalency.

    To obtain our main results, we need to following knowledgements owing to Airault and Bouali [1].

    Using the Faber polynomial expansion of function sA given in (1.1), s1=g may be given as

    r(w)=s1(w)=w+k=21kKkk1(a2,a3,)wk,

    where

    Kkk1=(k)!(2k+1)!(k1)!ak12+(k)![2(k+1)]!(k3)!ak32a3
    +(k)!(2k+3)!(k4)!ak42a4
    +(k)![2(k+2)]!(k5)!ak52[a5+(k+2)a23]
    +(k)!(2k+5)!(k6)!ak62[a6+(2k+5)a3a4]
    +j7akj2Vj,

    symbolically such term (k!)Γ(1k):=(k)(k1)(k2)(kN0,N:={1,2,3,}) and Vj with 7jk is a homologous polynomial in a2,a3,ak, [2]. Particularly, some initial terms of Kkk1 are

    K21=2a2,
    K32=3(2a22a3),
    K43=4(5a325a2a3+a4).

    Generally, for any pN:={1,2,3}, an expansion of Kpk is given, [1],

    Kpk=pak+p(p1)2D2k+p!(p3)!3!D3k++p!(pk)!(k)!Dkk,

    where Dpk=Dpk(a1,a2,a3,,ak), and by [26],

    Dmk(a1,a2,ak)=m=2m!i1!ik!ai11aikkformk

    while a1=1, and non-negative integers i1,,ik satisfying

    i1+i2+...+ik=m,
    i1+2i2+...+kik=k.

    It is obvious that Dkk(a1,a2,...ak)=ak1.

    As a result, for sWμ,qΣ(α,τ;φ) given by (1.1), we can write

    1+1τ[(1α)ζμqs(z)z+αq(ζμqs(z))1]=1+1τk=2[k,αq]ϕk1akzk (2.3)

    where

    [k,αq]=1+k1l=1αql.

    Theorem 4. For α1,μ>1,0<q<1, τ>0, let the function given by (1.1) sWμ,qΣ(α,τ;φ). If am=0 for 2mk1, then

    |ak|2τ[1+k1l=1αql]ϕk1.

    Proof. For analytic functions s given by (1.1), we get

    1+1τ[(1α)ζμqs(z)z+αq(ζμqs(z))1]=1+1τk=2[1+k1l=1αql]ϕk1akzk1 (2.4)

    and

    1+1τ[(1α)ζμqr(w)w+αq(ζμqr(w))1]=1+1τk=2[1+k1l=1αql]ϕk1bkwk1=1+1τk=2[1+k1l=1αql]ϕk1×1kKkk1(a2,a3,ak)wk1. (2.5)

    Moreover, the correlations (2.1) and (2.2) refer to the presence of Schwartz functions

    u(z)=k=2ckzk   and  ϑ(w)=k=2dkwk (2.6)

    so that

    1+1τ[(1α)ζμqs(z)z+αq(ζμqs(z))1]=φ(u(z)) (2.7)
    1+1τ[(1α)ζμqr(w)w+αq(ζμqr(w))1]=φ(ϑ(w)) (2.8)

    where

    φ(u(z))=1+k=1kn=1φnDnk(c1,c2,,ck)zk (2.9)
    φ(ϑ(w))=1+k=1kn=1φnDnk(d1,d2,,dk)wk. (2.10)

    Thus, from (2.4), (2.6) and (2.9) we have

    1τ[1+k1l=1αql]ϕk1ak=kn=1φnDnk(c1,c2,,ck),  (k2). (2.11)

    Similarly, by using (2.5), (2.6) and (2.10) we find that

    1τ[1+k1l=1αql]ϕk1bk=kn=1φnDnk(d1,d2,,dk),  (k2). (2.12)

    For an=0(2nk1), we get

    bk=ak

    and so

    1τ[1+k1l=1αql]ϕk1ak=φ1ck1,1τ[1+k1l=1αql]ϕk1ak=φ1dk1.

    When we take the absolute values of either of the above two equalities and using |φ1|2,|ck1|1 and |dk1|1, we obtain

    ak=|φ1ck1|τ|[1+k1l=1αql]ϕk1|=|φ1dk1|τ|[1+k1l=1αql]ϕk1|2τ[1+k1l=1αql]ϕk1

    which evidently completes the proof of theorem.

    We have the Corollary 5, when we choose τ=1 in Theorem 4.

    Corollary 5. For α1,μ>10<q<1, let s in the form (1.1) be in Wμ,qΣ(α;φ). If am=0 for 2mk1, then

    |ak|2[1+k1l=1αql]ϕk1.

    Comforting the coeefficient restricts produced in Theorem 4, we get coefficients given early of sWμ,qΣ(α,τ;φ) given below.

    Theorem 6. Let sWμ,qΣ(α,τ;φ) and for α1,μ>1, 0<q<1, τ>0. Then

    (i)|a2|min{2τ(1+αq)ϕ1,2τ(1+αq+αq2)ϕ2}
    (ii)|a3|min{4τ2(1+αq)2ϕ21+2|τ|(1+αq+αq2)ϕ2,6τ(1+αq+αq2)ϕ2}

    and

    (iii)|a32a22|4τ(1+αq+αq2)ϕ2.

    Proof. we obtain following equalities by replacing k by 2 and 3 in (2.11) and (2.12), respectively,

    1τ(1+αq)ϕ1a2=φ1c1 (2.13)
    1τ(1+αq+αq2)ϕ2a3=φ1c2+φ2c21 (2.14)
    1τ(1+αq)ϕ1a2=φ1d1 (2.15)
    1τ(1+αq+αq2)ϕ2(2a22a3)=φ1d2+φ2d21. (2.16)

    From (2.13) and (2.15), we obtain,

    d1=c1

    and taking their absolute values,

    |a2|=|φ1c1|τ|(1+αq)ϕ1|=|φ1d1|τ|(1+αq)ϕ1|2τ(1+αq)ϕ1. (2.17)

    Now, by adding (2.14) and (2.16), implies that

    2τ[(1+αq+αq2)ϕ2]a22=φ1(c2+d2)+φ2(c21+d21)

    or equivalently, (by taking the square roots and using Caratheodary Lemma)

    |a2|2τ(1+αq+αq2)ϕ2 (2.18)

    Next, in order to obtain the coefficient estimate of |a3|, we subtract (2.16) from (2.14). Thus we get

    2τ[τ](a3a22)=φ1(c2d2)+φ2(c21d21)

    or equivalently,

    |a3||a22|+|φ1(c2d2)|τ2|(1+αq+αq2)ϕ2|. (2.19)

    By replacing |a22| from (2.17) and (2.18) into (2.19), we get,

    |a3|4τ2(1+αq)2ϕ21+2τ(1+αq+αq2)ϕ2

    and

    |a3|6τ(1+αq+αq2)ϕ2.

    Finally, from (2.16), we deduce that (by Caratheodary Lemma)

    |a32a22|=|φ1d2+φ2d21|τ|(1+αq+αq2)ϕ2|4τ(1+αq+αq2)ϕ2.

    So, the proof is over.

    By letting q1 in Theorem 6, we get the Corollary 7.

    Corollary 7. Let s presented by (1.1) be in the family WμΣ(α,τ;φ) if am=0 for 2mk1, then

    (i)|a2|2τ(1+α)ϕ1,2τ(1+2α)ϕ2
    (ii)|a3|4τ2(1+α)2ϕ21+2τ(1+2α)ϕ2,6τ(1+2α)ϕ2

    and

    (iii)|a32a22|4τ(1+2α)ϕ2.

    By letting τ=1 in Corrollary 7, we obtain Corollary 8.

    Corollary 8. Let s indicated by (1.1) be in the family WμΣ(α;φ) if am=0 for 2mk1, then

    (i)|a2|2(1+α)ϕ1,2(1+2α)ϕ2
    (ii)|a3|4(1+α)2ϕ21+2(1+2α)ϕ2,6(1+2α)ϕ2

    and

    (iii)|a32a22|4(1+2α)ϕ2.

    The authors declare no conflict of interest.



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