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:z∈Cand|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(z∈D) |
D and hold the necessity ℜ(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 s−1 fulfilling
s−1(s(z))=z(z∈D) |
and
s(s−1(w))=w(|w|<r0(s)r0(s)≥14). |
Actually, the inverse function s−1 is denoted by
r(w)=s−1(w)=w−a2w2+(2a22−a3)w3−(5a32−5a2a3+a4)w4+⋯. | (1.2) |
If both s(z) and s−1(z) are univalent, we can say that, s∈A 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 s∈A is given by
∂qs(z)=s(qz)−s(z)(q−1)z,z≠0 | (1.4) |
and
∂qs(0)=s′(0). |
Thus we have
∂qs(z)=1+∞∑k=2[k,q]akzk−1 | (1.5) |
where [k,q] is presented by
[k,q]=1−qk1−q, [0,q]=0 | (1.6) |
and define the q-fractional by
[k,q]!={k∏n=1[n,q],k∈N1,k=0. | (1.7) |
Furthermore, Pochhammer symbol which is q−generalized for p≥0 is denoted by
[p,q]k={k∏n=1[p+n−1,q],k∈N1,k=0. | (1.8) |
In addition, as q→1−,[k,q]→k, if we select r(z)=zk, then we obtain
∂qr(z)=∂qzk=[k,q]zk−1=r′(z), |
where r′ is the ordinary derivative.
Recently, F−1q,μ+1(z), given with the following relation, was defined by Arif et al. (see[8])
F−1q,μ+1(z)∗Fq,μ+1(z)=z∂qs(z), (μ>−1) | (1.9) |
where
Fq,μ+1(z)=z+∞∑k=2[μ+1,q]k−1[k−1,q]!zk, z∈D. | (1.10) |
Due to the fact that series given in (1.10) is convergent absolutely in z∈D, by taking advantage of the characterization of q -derivative via convolution, one can define the integral operator ζμq:D→D by
ζμqs(z)=F−1q,μ+1(z)∗s(z)=z+∞∑k=2ϕk−1akzk, (z∈D) | (1.11) |
where
ϕk−1=[k,q]![μ+1,q]k−1. | (1.12) |
We note that
ζ0qs(z)=z∂qs(z),ζ′qs(z)=s(z) | (1.13) |
and
limq→1ζμqs(z)=z+∞∑k=2k!(μ+1)k−1akzk. | (1.14) |
Equation (1.14) means that the operator denoted by (1.11) reduces to the known Noor integral operator by getting q→1, 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 s∈Σ is known in the class Wμ,qΣ(α,τ;φ) if the requirements given below hold:
1+1τ[(1−α)ζμqs(z)z+α∂q(ζμqs(z))−1]≺φ(z)(z∈D), | (2.1) |
and
1+1τ[(1−α)ζμqr(w)w+α∂q(ζμqr(w))−1]≺φ(w)(w∈D) | (2.2) |
where (μ>−1,0<q<1, τ>0,α≥0) and s=r−1(w) is given by (1.2).
It is clear from Definition 3 that upon setting q→1−, for τ=1, α=1 and μ=1, one can easily see that s∈Σ is in
W1Σ(1,1;φ)=Hσ(φ) |
if the conditions given below hold true:
s′(z)≺φ(z)(z∈D), |
and
r′(w)≺φ(w)(w∈D), |
where r=s−1 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 s∈A given in (1.1), s−1=g may be given as
r(w)=s−1(w)=w+∞∑k=21kK−kk−1(a2,a3,…)wk, |
where
K−kk−1=(−k)!(−2k+1)!(k−1)!ak−12+(−k)![2(−k+1)]!(k−3)!ak−32a3 |
+(−k)!(−2k+3)!(k−4)!ak−42a4 |
+(−k)![2(−k+2)]!(k−5)!ak−52[a5+(−k+2)a23] |
+(−k)!(−2k+5)!(k−6)!ak−62[a6+(−2k+5)a3a4] |
+∑j≥7ak−j2Vj, |
symbolically such term (−k!)≡Γ(1−k):=(−k)(−k−1)(−k−2)⋯(k∈N0,N:={1,2,3,⋯}) and Vj with 7≤j≤k is a homologous polynomial in a2,a3,…ak, [2]. Particularly, some initial terms of K−kk−1 are
K−21=−2a2, |
K−32=3(2a22−a3), |
K−43=−4(5a32−5a2a3+a4). |
Generally, for any p∈N:={1,2,3…}, an expansion of Kpk is given, [1],
Kpk=pak+p(p−1)2D2k+p!(p−3)!3!D3k+…+p!(p−k)!(k)!Dkk, |
where Dpk=Dpk(a1,a2,a3,…,ak), and by [26],
Dmk(a1,a2,…ak)=∞∑m=2m!i1!…ik!ai11…aikkform≤k |
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 s∈Wμ,qΣ(α,τ;φ) given by (1.1), we can write
1+1τ[(1−α)ζμqs(z)z+α∂q(ζμqs(z))−1]=1+1τ∞∑k=2[k,αq]ϕk−1akzk | (2.3) |
where
[k,αq]=1+k−1∑l=1αql. |
Theorem 4. For α≥1,μ>−1,0<q<1, τ>0, let the function given by (1.1) s∈Wμ,qΣ(α,τ;φ). If am=0 for 2≤m≤k−1, then
|ak|≤2τ[1+k−1∑l=1αql]ϕk−1. |
Proof. For analytic functions s given by (1.1), we get
1+1τ[(1−α)ζμqs(z)z+α∂q(ζμqs(z))−1]=1+1τ∞∑k=2[1+k−1∑l=1αql]ϕk−1akzk−1 | (2.4) |
and
1+1τ[(1−α)ζμqr(w)w+α∂q(ζμqr(w))−1]=1+1τ∞∑k=2[1+k−1∑l=1αql]ϕk−1bkwk−1=1+1τ∞∑k=2[1+k−1∑l=1αql]ϕk−1×1kK−kk−1(a2,a3,…ak)wk−1. | (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[(1−α)ζμqs(z)z+α∂q(ζμqs(z))−1]=φ(u(z)) | (2.7) |
1+1τ[(1−α)ζμqr(w)w+α∂q(ζμqr(w))−1]=φ(ϑ(w)) | (2.8) |
where
φ(u(z))=1+∞∑k=1k∑n=1φnDnk(c1,c2,…,ck)zk | (2.9) |
φ(ϑ(w))=1+∞∑k=1k∑n=1φnDnk(d1,d2,…,dk)wk. | (2.10) |
Thus, from (2.4), (2.6) and (2.9) we have
1τ[1+k−1∑l=1αql]ϕk−1ak=k∑n=1φnDnk(c1,c2,…,ck), (k≥2). | (2.11) |
Similarly, by using (2.5), (2.6) and (2.10) we find that
1τ[1+k−1∑l=1αql]ϕk−1bk=k∑n=1φnDnk(d1,d2,…,dk), (k≥2). | (2.12) |
For an=0(2≤n≤k−1), we get
bk=−ak |
and so
1τ[1+k−1∑l=1αql]ϕk−1ak=φ1ck−1,−1τ[1+k−1∑l=1αql]ϕk−1ak=φ1dk−1. |
When we take the absolute values of either of the above two equalities and using |φ1|≤2,|ck−1|≤1 and |dk−1|≤1, we obtain
ak=|φ1ck−1|τ|[1+k−1∑l=1αql]ϕk−1|=|φ1dk−1|τ|[1+k−1∑l=1αql]ϕk−1|≤2τ[1+k−1∑l=1αql]ϕk−1 |
which evidently completes the proof of theorem.
We have the Corollary 5, when we choose τ=1 in Theorem 4.
Corollary 5. For α≥1,μ>−10<q<1, let s in the form (1.1) be in Wμ,qΣ(α;φ). If am=0 for 2≤m≤k−1, then
|ak|≤2[1+k−1∑l=1αql]ϕk−1. |
Comforting the coeefficient restricts produced in Theorem 4, we get coefficients given early of s∈Wμ,qΣ(α,τ;φ) given below.
Theorem 6. Let s∈Wμ,qΣ(α,τ;φ) and for α≥1,μ>−1, 0<q<1, τ>0. Then
(i)|a2|≤min{2τ(1+αq)ϕ1,2√τ√(1+αq+αq2)ϕ2} |
(ii)|a3|≤min{4τ2(1+αq)2ϕ21+2|τ|(1+αq+αq2)ϕ2,6τ(1+αq+αq2)ϕ2} |
and
(iii)|a3−2a22|≤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(2a22−a3)=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|≤2√τ√(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](a3−a22)=φ1(c2−d2)+φ2(c21−d21) |
or equivalently,
|a3|≤|a22|+|φ1(c2−d2)|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)
|a3−2a22|=|φ1d2+φ2d21|τ|(1+αq+αq2)ϕ2|≤4τ(1+αq+αq2)ϕ2. |
So, the proof is over.
By letting q→1− 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 2≤m≤k−1, then
(i)|a2|≤2τ(1+α)ϕ1,2√τ√(1+2α)ϕ2 |
(ii)|a3|≤4τ2(1+α)2ϕ21+2τ(1+2α)ϕ2,6τ(1+2α)ϕ2 |
and
(iii)|a3−2a22|≤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 2≤m≤k−1, 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)|a3−2a22|≤4(1+2α)ϕ2. |
The authors declare no conflict of interest.
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