In this paper, we define new subclasses of analytic functions related to a modified sigmoid function and analytic univalent function. Then, we attempt to investigate the upper bounds of the third and fourth Hankel determinant in the special case. Further, bound on third Hankel determinant of its inverse function is also investigated. In addition, we attempt to obtain the Fekete-Szegö inequality for the classes. Then, we estimate the bounds of initial coefficients for the function belongs to some kind of new subclasses when its inverse function also belongs to these new subclasses.
Citation: Wenzheng Hu, Jian Deng. Hankel determinants, Fekete-Szegö inequality, and estimates of initial coefficients for certain subclasses of analytic functions[J]. AIMS Mathematics, 2024, 9(3): 6445-6467. doi: 10.3934/math.2024314
[1] | Mohammad Faisal Khan, Jongsuk Ro, Muhammad Ghaffar Khan . Sharp estimate for starlikeness related to a tangent domain. AIMS Mathematics, 2024, 9(8): 20721-20741. doi: 10.3934/math.20241007 |
[2] | Muhammad Ghaffar Khan, Nak Eun Cho, Timilehin Gideon Shaba, Bakhtiar Ahmad, Wali Khan Mashwani . Coefficient functionals for a class of bounded turning functions related to modified sigmoid function. AIMS Mathematics, 2022, 7(2): 3133-3149. doi: 10.3934/math.2022173 |
[3] | Muhammad Ghaffar Khan, Sheza.M. El-Deeb, Daniel Breaz, Wali Khan Mashwani, Bakhtiar Ahmad . Sufficiency criteria for a class of convex functions connected with tangent function. AIMS Mathematics, 2024, 9(7): 18608-18624. doi: 10.3934/math.2024906 |
[4] | Muhammmad Ghaffar Khan, Wali Khan Mashwani, Lei Shi, Serkan Araci, Bakhtiar Ahmad, Bilal Khan . Hankel inequalities for bounded turning functions in the domain of cosine Hyperbolic function. AIMS Mathematics, 2023, 8(9): 21993-22008. doi: 10.3934/math.20231121 |
[5] | Pinhong Long, Xing Li, Gangadharan Murugusundaramoorthy, Wenshuai Wang . The Fekete-Szegö type inequalities for certain subclasses analytic functions associated with petal shaped region. AIMS Mathematics, 2021, 6(6): 6087-6106. doi: 10.3934/math.2021357 |
[6] | Huo Tang, Muhammad Abbas, Reem K. Alhefthi, Muhammad Arif . Problems involving combinations of coefficients for the inverse of some complex-valued analytical functions. AIMS Mathematics, 2024, 9(10): 28931-28954. doi: 10.3934/math.20241404 |
[7] | Jianhua Gong, Muhammad Ghaffar Khan, Hala Alaqad, Bilal Khan . Sharp inequalities for q-starlike functions associated with differential subordination and q-calculus. AIMS Mathematics, 2024, 9(10): 28421-28446. doi: 10.3934/math.20241379 |
[8] | Daud Mohamad, Nur Hazwani Aqilah Abdul Wahid, Nurfatin Nabilah Md Fauzi . Some properties of a new subclass of tilted star-like functions with respect to symmetric conjugate points. AIMS Mathematics, 2023, 8(1): 1889-1900. doi: 10.3934/math.2023097 |
[9] | Huo Tang, Shahid Khan, Saqib Hussain, Nasir Khan . Hankel and Toeplitz determinant for a subclass of multivalent q-starlike functions of order α. AIMS Mathematics, 2021, 6(6): 5421-5439. doi: 10.3934/math.2021320 |
[10] | Zhen Peng, Muhammad Arif, Muhammad Abbas, Nak Eun Cho, Reem K. Alhefthi . Sharp coefficient problems of functions with bounded turning subordinated to the domain of cosine hyperbolic function. AIMS Mathematics, 2024, 9(6): 15761-15781. doi: 10.3934/math.2024761 |
In this paper, we define new subclasses of analytic functions related to a modified sigmoid function and analytic univalent function. Then, we attempt to investigate the upper bounds of the third and fourth Hankel determinant in the special case. Further, bound on third Hankel determinant of its inverse function is also investigated. In addition, we attempt to obtain the Fekete-Szegö inequality for the classes. Then, we estimate the bounds of initial coefficients for the function belongs to some kind of new subclasses when its inverse function also belongs to these new subclasses.
Let S denote the class of univalent functions which are analytic in the open unit disk D={z∈C:|z|<1} of the form
f(z)=z+∞∑n=2anzn(z∈D). | (1.1) |
Let P represent a class of analytic functions within the unit disk D of the form
p(z)=1+∞∑n=1cnzn(z∈D) | (1.2) |
and satisfy the condition of ℜ(p(z))>0. It is easy to know from the conclusion of [1], for p(z)∈P, there exists a Schwarz function w(z), making
p(z)∈P⇔p(z)=1+w(z)1−w(z). |
In 1976, Noonan and Thomas [2] defined the qth Hankel determinant for a function f∈S of form (1.1) as
Hq,n(f)=|anan+1⋯an+q−1an+1an+2⋯an+q⋮⋮⋮⋮an+q−1an+q⋯an+2q−2|, |
where a1=1,n≥1,q≥1. In particular, we have
H2,1(f)=a3−a22, |
H2,2(f)=a2a4−a23, |
H3,1(f)=a3(a2a4−a23)−a4(a4−a2a3)+a5(a3−a22) |
and
H4,1(f)=a7H3,1(f)−a6δ1+a5δ2−a4δ3, |
where
δ1=a3(a2a5−a3a4)−a4(a5−a2a4)+a6(a3−a22), |
δ2=a3(a3a5−a24)−a5(a5−a2a4)+a6(a4−a2a3), |
δ3=a4(a3a5−a24)−a5(a2a5−a3a4)+a6(a2a4−a23). |
Next, we recall the definition of subordination. We assume that f1 and f2 are two analytic functions in D. Then, we say that the function f1 is subordinate to the function f2, as we write f1(z)≺f2(z), for all z∈D. Then, there exists a Schwarz function w(z) with w(0)=0 and |w(z)|<1 to satisfy
f1(z)=f2(w(z)). |
Now, we consider the following class S∗(g) as follows:
S∗(g)={f∈S:zf′(z)f(z)≺g(z)}, | (1.3) |
where g is an analytic univalent function with positive real part in D, and g maps D onto a region starlike with respect to g(0)=1, g′(0)>0, and is symmetric about the real axis. The class S∗(g) was introduced by Ma and Minda [3]. If we vary the function g on the right side of (1.3), we will obtain different results. In recent years, many researchers have also conducted a lot of research on this and obtained a series of conclusions. Some of them are as follows:
(1) For g=21+e−z, which was defined in [4].
(2) For g=√1+z, it has been further studied in [5].
(3) For g=1+43z+23z2, it was introduced in [6] and further investigated in [7].
(4) For g=ez, it was defined and studied in [8].
(5) For g=z+√1+z2, the class is denoted by S∗l, and it was further studied in [9].
(6) For g=1+sinh−1z, the class S∗p=S∗(1+sinh−1z) was studied by Kumar and Arora [10].
(7) For g=coshz, the class S∗cosh=S∗(g(z)) was introduced by Alotaibi et al. [11].
The Fekete-Szegö inequality is one of the inequalities for the coefficients of univalent analytic functions found by Fekete and Szegö. The Fekete-Szegö inequality of various analytic functions has been studied by many researchers in the last few decades, for example, Huo Tang defined certain class of analytic functions related to the sine function (see [12])
f′(ζ)θ(ζf′(ζ)f(ζ))1−θ≺1+sin(ζ);(f∈S,0≤θ≤1) |
and investigated the upper bound of the second Hankel determinant and the Fekete-Szegö inequality for functions in this class. Many papers have been devoted to researching the Fekete-Szegö inequality for various sub-class functions (see [13,14]). Therefore, the study of the Fekete-Szegö inequality for different analytic functions is valuable and of great significance.
In recent years, many papers have been devoted to finding the upper bounds of Hankel determinants for various sub-classes of analytic functions as well. For the basics and preliminaries, the readers are advised to see the academic achievements in [15,16,17,18]. Guangadharan studied a class of bounded turning functions related to the three leaf function in [19]. From this, it can be seen that the research on Hankel determinants of various analytic functions has become popular. Therefore, it is an interesting and hot topic to investigate the Hankel determinants for various classes of analytic functions. In addition, it is worth mentioning that a class of star like functions associated with the modified sigmoid function was defined by Goel and Kumar [20],
SSG={f∈S:zf′(z)f(z)≺21+e−z}. |
Apart from the above, the coefficient bounds for certain analytic functions have been studied by many researchers, see [21,22,23,24,25]. Further, many star like functions have been defined and studied as well, see [26,27,28,29]. Not long ago, another class of analytic functions associated with the modified sigmoid function was defined and studied by Muhammad Ghaffar Khan [4],
RSG={f∈S:f′(z)≺21+e−z}. |
It is well known that for each univalent function f∈S, there is an inverse function f−1(w) which can be defined in (|w|<r;r≥14), where
f−1(w)=w−a2w2+(2a22−a3)w3−(5a32−5a2a3+a4)w4+⋅⋅⋅. |
A function f∈S is said to be bi-univalent in D if there exists a function g∈S such that g(z) is a univalent extension of f−1 to D. Brannan [30] studied classes of bi-univalent functions and obtained estimates for their initial coefficients. Many classes of bi-univalent funtions were introduced and further studied in the past few years. Inspired by all the aforementioned works, in this paper we investigate another certain class of analytic functions H(λ,ψ), which are related to the modified sigmoid function, and discuss the upper bound of the fourth-order Hankel determinant in special cases, here we use another method to obtain improved results compared to [20]. And we also obtain the upper bound of third-order Hankel determinant of its inverse function. Furthermore, we discuss the Fekete-Szegő inequality for functions in this class when λ∈[0,1] and ψ=21+e−z. Finally, we estimate the upper bounds of the initial coefficients for functions in this class when λ∈[0,1], ψ(0)=1, and ψ′(0)>0, where its inverse function f−1 also belongs to this class.
Definition 1.1. Assume that f∈S, 0≤λ≤1, (f′(z))1−λ and (2zf′(z)f(z)−f(−z))λ are analytic in D with f′(z)≠0, and f(z)≠f(−z) for all z∈D∖{0}. Furthermore, (f′(z))λ = 1 at z=0, ψ(z) is a univalent and analytic function. Then, f(z) is said to be in the class H(λ,ψ) if the following condition is satisfied:
(1−λ)(f′(z))1−λ+λ(2zf′(z)f(z)−f(−z))λ≺ψ(z). |
For convenience, we denote
H(λ)=H(λ,21+e−z). |
Remark 1.1. For any λ∈[0,1], we have that f(z)=z∈H(λ) always holds.
Below we will evaluate bounds of the first six initial coefficients and non-sharp bound of the third Hankel determinant for functions belonging to H(1).
Theorem 2.1. Let f∈H(1) and be of form (1.1). Then,
|a2|≤14, | (2.1) |
|a3|≤14, | (2.2) |
|a4|≤18, | (2.3) |
|a5|≤18, | (2.4) |
|a6|≤731576, | (2.5) |
|a7|≤388937241920. | (2.6) |
The first four inequalities are sharp.
We need the following lemmas to prove the above theorem:
Lemma 2.1. [4] Let p∈P, then |cn|≤2.
Lemma 2.2. [17] Let p∈P, then for all n,m∈N, if 0≤ζ≤1, there is |cm+n−ζcmc1|≤2. If ζ<0 or ζ>1, there is |cm+n−ζcmc1|≤2|2ζ−1|.
Lemma 2.3. [4] Let p∈P, then
|αc31−βc1c2+γc3|≤2|α|+2|β−2α|+2|α−β+γ|, |
where α, β and γ are real numbers.
Lemma 2.4. [4] Let α, β, γ, and ζ satisfy the inequalities 0<γ<1,0<β<1, and
8β(1−β)[(γζ−2α)2+(γ(β+γ)−ζ)2]+γ(1−γ)(ζ−2βγ)2≤4γ2(1−γ)2β(1−β). |
If p∈P, then
|αc41+βc22+2γc1c3−32ζc21c2−c4|≤2. |
Proof. If f∈H(1), there exists a Schwarz function w(z) to satisfy
2zf′(z)f(z)−f(−z)=21+e−w(z). |
Also, if p∈P, it can be written in terms of the Schwarz function w(z) as
p(z)=1+c1z+c2z2+c3z3+⋅⋅⋅=1+w(z)1−w(z), |
or equivalently,
w(z)=p(z)−1p(z)+1=12c1z+(12c2−14c21)z2+(18c31−12c1c2+12c3)z3+⋅⋅⋅. | (2.7) |
Now, we set
2zf′(z)f(z)−f(−z)=1+b1z+b2z2+b3z3+b4z4+b5z5+b6z6+⋅⋅⋅=21+e−w(z). | (2.8) |
In addition,
2zf′(z)f(z)−f(−z)=1+2a2z+3a3z2+5a5z4+6a6z5+7a7z6+⋅⋅⋅1+a3z2+a5z4+a7z6+⋅⋅⋅. | (2.9) |
Using (2.8) and (2.9), we can get
b1=2a2, | (2.10) |
b2=2a3, | (2.11) |
b3=4a4−2a2a3, | (2.12) |
b4=4a5−2a23, | (2.13) |
b5=6a6−4a3a4+2a2a23−2a2a5, | (2.14) |
b6=6a7−4a3a5+2a23−2a3a5. | (2.15) |
Substituting (2.7) into the right side of (2.8), by simplifying, using (2.10)–(2.15), and comparing the coefficients on both sides of the equation, we can get
a2=18c1, | (2.16) |
a3=12(c24−c218), | (2.17) |
a4=14(124c31−732c1c2+c34), | (2.18) |
a5=−116(116c41−916c21c2+c1c3+38c22−c4), | (2.19) |
a6=16b5+23a3a4−13a2a23+13a2a5, | (2.20) |
a7=16b6+a3(3a5−a23)3+a3a53, | (2.21) |
where
b5=13072(−5c61+122c41c2−288c31c3−432c21c22+528c21c4+1056c1c2c3−768c1c5+176c32−768c2c4−384c23+768c6), |
b6=15160960(−2537c71−50400c51c2+204960c41c3+409920c31c22−483840c4c31−1451520c21c2c3+887040c21c5−483840c1c32+1774080c1c2c4+887040c1c23−1290240c1c6+887040c22c3−1290240c2c5−1290240c3c4+1290240c7). |
Applying Lemma 2.1, we have
|a2|≤14. |
The above inequality is sharp with extremal function f(z)=∫z021+e−tdt.
|a3|=18|c2−12c21|≤14. |
The above inequality is sharp for the function p(z)=(1+z2)/(1−z2).
Applying Lemma 2.3, we have
|a4|≤14[2|124|+2|732−112|+2|124−732+14|]=18. |
The above inequality is sharp with extremal function f(z)=∫z021+e−t3dt.
Applying Lemma 2.4, we have
|a5|=|116(116c41−916c21c3+c1c3+38c22−c4)|≤18. |
The above inequality is sharp for the function p(z)=(1+z4)/(1−z4).
Applying the triangle inequality, we have
|16b5|≤118432(122|c1|4|c2−5122c21|+1056|c1||c3||c2−311c21|+528|c1|2|c4−911c22|+768|c6−c1c5|+768|c2||c4−8889c22|+384|c3|2). |
By applying Lemmas 2.1 and 2.2, we have
|16b5|≤355288, |
and then applying the triangle inequality and (2.1)–(2.4), we have
|23a3a4−13a2a23+13a2a5|≤23|a3||a4|+13|a2||a3|2+13|a2||a5|≤7192, |
and from (2.20) we can obtain
|a6|≤355288+7192=731576. |
By applying triangle inequality, we have
|16b6|≤130965760(20965760|c1|4|c3−105427c1c2|+483840|c1|3|c4−6172c21|+1290240|c1||c6−1116c1c5|+1774080|c1||c2||c4−911c1c3|+887040|c2|2|c3−611c1c2|+1290240|c7−c2c5|+1290240|c3||c4−1116c1c3|+2537|c1|7). |
Then, from (2.2) and Lemmas 2.1, 2.2, and 2.4, we have
|16b6|≤381377241920, |
|a3(2a5−a23)3|=124|a3||332c41+12c22+c1c3−1116c21c2−c4|≤148. |
From (2.2) and (2.4), we have
|a3a53|≤196. |
Then, applying the triangle inequality and (2.21), we can get
|a7|≤381377241920+148+196=388937241920. |
This completes our proof.
Theorem 2.2. If f of the form (1.1) belongs to H(1), then
|a3−a22|≤14. |
The result is sharp for the function p(z)=(1+z2)/(1−z2).
Proof. Using (2.16), (2.17), and Lemma 2.2, we have
|a3−a22|=18|c2−58c21|≤14. |
Theorem 2.3. If f of the form (1.1) belongs to H(1), then
|a2a3−a4|≤18. |
The result is sharp with the extremal function f(z)=∫z021+e−t3dt.
Proof. Using (2.16)–(2.18), we can get
|a2a3−a4|=|7384c31−9128c1c2+116c3|. |
Applying Lemma 2.3,
|7384c31−9128c1c2+116c3|≤2|7384|+2|9128−7192|+2|7384−9128+116|=18. |
Theorem 2.4. If f of the form (1.1) belongs to H(1), then
|a2a4−a23|≤116. |
The result is sharp with the extremal function f(z)=∫z021+e−t3dt.
Proof. Using (2.16)–(2.18), we can get
|a2a4−a23|=164|−16c41+916c21c2+12c1c3−c22|. |
Now, in order to get the desired bound, we shall prove that
|−16c41+916c21c2+12c1c3−c22|≤4. | (2.22) |
Next we will use the following Lemma:
Lemma 2.5. [17] Let p∈P. Then, there exists some x, y with |x|≤1,|y|≤1 such that
2c2=c21+x(4−c21), |
4c3=c31+2c1x(4−c21)−(4−c21)c1x2+2(4−c21)(1−|x|2)y. |
Using the invariant property under rotation, we can assume that c=c1∈[0,2], and then from Lemma 2.5, substituting the expression for c2, c3 and simplifying, we can obtain
−16c41+916c21c2+12c1c3−c22=−196c4+132c2(4−c2)x−14(4−c2)(4−12c2)x2+14c(4−c2)(1−|x|2)y. |
If c=0, there is
|−16c41+916c21c2+12c1c3−c22|=4|x|2≤4. |
If c=2, there is
|−16c41+916c21c2+12c1c3−c22|=16. |
Next, we will discuss the case of c∈(0,2). At this time,
−16c41+916c21c2+12c1c3−c22=14c(4−c2)[px2+qx+t+(1−|x|2)y], |
where
p=c2−82c,q=c8,t=−c324(4−c2), |
and then we denote
I=14c(4−c2)[px2+qx+t+(1−|x|2)y], |
where p<0,q>0, and t<0 always holds due to the fact that c∈(0,2). Then, by using the triangle inequality, we have
|I|≤14c(4−c2)(1−|x|2+|p||x|2+|q||x|+|t|)=14c(4−c2)[−(p+1)|x|2+q|x|−t+1]. |
Since q2(p+1)<0 always holds, we can obtain
|I|≤14c(4−c2)(−p+q−t)=548c4−118c2+4=f(c). |
By computation, it can be revealed that
f(c)<max{f(0),f(2)}=4. |
In summary, |I|≤4, that is, (2.22) holds, which evidently yields
|−16c41+916c21c2+12c1c3−c22|≤4. |
This completes the proof.
Theorem 2.5. If f of the form (1.1) belongs to H(1), then
|H3,1(f)|≤116. |
Proof.
H3,1(f)=a3(a2a4−a23)−a4(a4−a2a3)+a5(a3−a22). |
By using the triangle inequality, we have
|H3,1(f)|≤|a3||a2a4−a23|+|a4||a4−a2a3|+|a5||a3−a22|. |
According to Theorem 2.1, we have
|a3|≤14,|a4|≤18,|a5|≤18. |
According to Theorems 2.2–2.4, we have
|a2a4−a23|≤116,|a4−a2a3|≤18,|a3−a22|≤14. |
Therefore,
|H3,1(f)|≤116. |
Below we will evaluate the non-sharp bound of the fourth determinant for functions belonging to H(1).
Theorem 3.1. If f of the form (1.1) belongs to H(1), then
|a2a5−a3a4|≤116. |
Proof. Using (2.16)–(2.19), we can get
|a2a5−a3a4|=|16144c51−13072c31c2−1256c21c3+1256c1c22+1128c1c4−1128c2c3|. |
Then, by applying the triangle inequality, we have
|a2a5−a3a4|≤13072|c31(c2−c212)|+1128|c2(c3−c1c22)|+1128|c1(c4−c1c32)|. |
We denote |c1|=c, and from Lemmas 2.1 and 2.2 we can obtain
|c31(c2−c212)|≤c3(2−12c2),1128|c2(c3−c1c22)|≤132,1128|c1(c4−c1c32)|≤c64. |
Thus,
|a2a5−a3a4|≤13072c3(2−c22)+c64+132=G(c), |
G′(c)=−5c46144+c2512+164≥0c∈[0,2]. |
Therefore,
G(c)≤G(2)=116. |
This completes the proof.
Theorem 3.2. If f of the form (1.1) belongs to H(1), then
|a5−a2a4|≤18. |
Proof. By using (2.16), (2.18), and (2.19), we have
|a5−a2a4|=116|112c41−4364c21c2+98c1c3+38c22−c4|. |
By applying Lemma 2.4, we can get the sharp result for the function p(z)=(1+z4)/(1−z4).
Theorem 3.3. If f of the form (1.1) belongs to H(1), then
|a3a5−a24|≤689+144√39216. |
Proof. Using (2.17)–(2.19), we can obtain
|a3a5−a24|=|536864c61−1912288c41c2+1384c31c3+4716384c21c22−1256c21c4−11024c1c2c3−31024c32+1128c2c4−1256c23|. |
By applying the triangle inequality, we get
|a3a5−a24|≤536864|c1|6+149152|c2||76c41−141c21c2+48c1c3+144c22|+1384|c3||c31−32c3|+1128|c4||c2−12c21|. |
In order to get the desired bound, we shall prove that
|76c41−141c21c2+48c1c3+144c22|≤856. |
Using the invariant property under rotation, we can assume that c=c1∈[0,2], and then from Lemma 2.5, substituting the expression for c2, c3 and simplifying, we have
76c41−141c21c2+48c1c3+144c22=1072c4+512c2(4−c2)x+48(4−c2)(3−c2)x2+24c(4−c2)(1−|x|2)y. |
If c=0,
|76c41−141c21c2+48c1c3+144c22|=576. | (3.1) |
If c=2,
|76c41−141c21c2+48c1c3+144c22|=856. | (3.2) |
If c≠0 and c≠2, we have
76c41−141c21c2+48c1c3+144c22=24c(4−c2)[p+qx+tx2+(1−|x|2)y], |
where
p=107c348(4−c2),q=17c16,t=6−2c2c. |
p,q>0 always holds due to the fact that c∈(0,2). Then, by using the triangle inequality, we have
|76c41−141c21c2+48c1c3+144c22|≤24c(4−c2)(1−|x|2+p+q|x|+|t||x|2). |
We denote
I=24c(4−c2)(1−|x|2+p+q|x|+|t||x|2). |
For suitability, we divide the calculation in five cases:
Case (I). t≤0 if and only if √3=c1≤c<2. At this time,
I=24c(4−c2)[−(1+t)|x|2+q|x|+p+1], |
and when c1≤c<c2, there is q2(1+t)<1, where c2=16+8√24781. Then, we have
I≤24c(4−c2)−4(1+t)p−q2−4(1+t)+24c(4−c2)=107c42+867128c42+c3+2c+24c(4−c2)=f1(c). |
By computation, it can be revealed that
f1(c)<856,c∈[c1,c2). | (3.3) |
Case (II). For c∈[c2,2), there is q2(1+t)≥1, and we then have
I≤24c(4−c2)(p+q−t)=−20c4+438c2−576=f2(c). |
By computation, we have
f2(c)<856,c∈[c2,2). | (3.4) |
Case (III). For c1>c>c3=−16+8√14547, we have
I=24c(4−c2)[(t−1)|x|2+q|x|+p+1], |
where q2(1−t)<1, and we then obtain
I≤24c(4−c2)4(t−1)p−q24(t−1)+24c(4−c2)=107c42−867128c42−c3−2c+24c(4−c2)=f3(c). |
Now, computation reveals that
f3(c)<856,c∈(c3,c1). | (3.5) |
Case (IV). For c3≥c>c4, where c4=32, there is q2(1−t)>1. We can get
I≤24c(4−c2)(t+p+q)=76c4−234c2+576=f4(c). |
A computation shows that
f4(c)<856,c∈(c4,c3]. | (3.6) |
Case (V). For the case of c∈(0,c4], we have
I=24c(4−c2)[(t−1)|x|2+q|x|+p+1], |
where t−1>0 holds for c∈(0,32). Thus, we have
I≤max{24c(4−c2)(p+1),24c(4−c2)(p+q+t)}, |
or, equivalently,
I≤max{107c42+24c(4−c2),76c4−234c2+576}. |
Now, we denote
g1(c)=107c42+24c(4−c2),g2(c)=76c4−234c2+576 |
g′1(c)=314c3−72c2+96, |
g″1(c)=144c(471c72−1). |
g′1(c) attains its minimum at c0=72471, g′1(c0)>0, which evidently yields that g′1(c)>0 holds for c∈(0,32). Therefore, g1(c)<g1(32)=333.84375. On the other hand,
g2(c)<max{g2(0),g2(32)}=576. |
Thus,
I<576,c∈(0,c4]. | (3.7) |
From (3.11)–(3.17), we conclude that I≤856, which implies
|76c41−141c21c2+48c1c3+144c22|≤856. | (3.8) |
Next, we will use the following lemma:
Lemma 3.1. Let p(z)=1+c1z+c2z2+c3z3+⋅⋅⋅∈P. Then, for any real number μ,
|μc3−c31|≤{2|μ−4|(μ≤43),2μ√μμ−1(43<μ). |
By Lemmas 2.1, 2.2, and 3.1, we can obtain
|536864c61|≤5576,149152|c2||76c41−141c21c2+48c1c3+144c22|≤1073072. | (3.9) |
1384|c3||c31−32c3|≤√364,1128|c4||c2−12c21|≤132. | (3.10) |
From (3.9) and (3.10), we have
|a3a5−a24|≤689+144√39216. |
This completes our proof.
Theorem 3.4. If f of the form (1.1) belongs to H(1), then
|H4,1(f)|≤215139562371589120+3√34096. |
Proof. We can write H4,1(f) as
H4,1(f)=a7H3,1(f)−a6δ1+a5δ2−a4δ3, |
where
δ1=a3(a2a5−a3a4)−a4(a5−a2a4)+a6(a3−a22), |
δ2=a3(a3a5−a24)−a5(a5−a2a4)+a6(a4−a2a3), |
δ3=a4(a3a5−a24)−a5(a2a5−a3a4)+a6(a2a4−a23). |
By applying Theorems 2.1–2.5, 3.1–3.3, and the triangle inequality, we have
|H4,1(f)|≤|a7||H3,1(f)|+|a6||δ1|+|a5||δ2|+|a4||δ3|, | (3.11) |
|a7||H3,1|≤388937241920×116=3889373870720, | (3.12) |
|δ1|≤|a3||a2a5−a3a4|+|a4||a5−a2a4|+|a6||a3−a22|≤8032304, | (3.13) |
|δ2|≤|a3||a3a5−a24|+|a5||a5−a2a4|+|a6||a4−a2a3|≤237112288+√3256, | (3.14) |
|δ3|≤|a4||a3a5−a24|+|a5||a2a5−a3a4|+|a6||a2a4−a23|≤2371+48√324576. | (3.15) |
Thus, from (3.11)–(3.15), we obtain
|H4,1(f)|≤215139562371589120+3√34096. |
Theorem 4.1. If the function f∈H(1) given by (1.1) and f−1(w)=w+∑∞n=2dnwn is the analytic continuation to D of the inverse function of f with |w|<r0, where r0≥14 is the radius of the Koebe domain, then
|d2|≤14, | (4.1) |
|d3|≤14, | (4.2) |
|d4|≤65384, | (4.3) |
|d5|≤167256. | (4.4) |
The first three inequalities are sharp.
Proof. If
f−1(w)=w+∞∑n=2dnwn |
is the inverse function of f, it can be seen that
f−1(f(z))=f(f−1(z))=z. |
Equivalently,
∞∑n=1dn(z+∞∑k=2dkwk)n=z(d1=1). | (4.5) |
By comparing the coefficients on both sides of (4.5), we can obtain
d2=−a2, | (4.6) |
d3=2a22−a3, | (4.7) |
d4=−(5a32−5a2a3+a4), | (4.8) |
d5=14a42−21a22a3+6a2a4+3a23−a5. | (4.9) |
Applying Lemmas 2.1 and 2.2, (2.16), and (2.17), we have
|d2|=|a2|=|18c1|≤14, |
|d3|=18|c2−34c21|≤14. |
Applying Lemma 2.3 and (2.16)–(2.18), we have
|d4|=|911536c31−17128c1c2+116c3|≤2⋅|911536|+2⋅|17128−91768|+2⋅|911536−17128+116|=65384, |
|d5|=|972048c41−21128c21c2+764c1c3+9128c22−116c4|. |
By applying the triangle inequality, we can get
|d5|≤|972048c41−21128c21c2+764c1c3|+|9128c22−116c4|. |
Using Lemmas 2.1 and 2.3, we have
|972048c41−21128c21c2+764c1c3|=|c1||972048c31−21128c1c2+764c3|≤127256. |
Using Lemma 2.2, we obtain
|9128c22−116c4|=116|c4−98c22|≤532. |
Therefore,
|d5|≤127256+532=167256. |
This completes the proof.
Theorem 4.2. If the function f∈H(1) given by (1.1) and f−1(w)=w+∑∞n=2dnwn is the analytic continuation to D of the inverse function of f with |w|<r0, where r0≥14 is the radius of the Koebe domain, then
|H3,1(f−1)|≤34171147456. |
Proof. From Theorem 3.2, we have
|d3−d22|=|a22−a3|≤14. | (4.10) |
Applying (4.6)–(4.8) and (2.16)–(2.18),
|d2d3−d4|=|3a32−4a2a3+a4|=|731536c31−15128c1c2+116c3|. |
Using Lemma 2.3,
|d2d3−d4|≤2|731536|+2|15128−73768|+2|731536−15128+116|=59384. | (4.11) |
Applying (4.6)–(4.8) and (2.16)–(2.18),
|d2d4−d23|=|a42−a22a3+a2a4−a23|=164|17192c41+c22−716c21c2−12c1c3|. |
We denote |c1|=c∈[0,2],|x|=t∈[0,1], and referring to Lemma 2.5, we have
|c2|≤c2+t(4−c2)2,|c3|≤c34+c(4−c2)t2+(4−c2)ct24+(4−c2)(1−t2)2. |
Using the triangle inequality, we have
|17192c41+c22−716c21c2−12c1c3|≤131192c4+(4−c2)c4+(c+2)(c+4)(c−2)28t2+31c2(4−c2)32t=F(c,t). |
∂F∂t=(c+2)(c+4)(c−2)24t+31c2(4−c2)32>0. |
Therefore,
F(c,t)≤F(c,1)=−31192c4+198c2+4=G(c), |
G′(c)=194c(1−31228c2)≥0. |
This leads to
G(c)≤G(2)=13112, |
|d2d4−d23|≤13112⋅164=131768. | (4.12) |
Applying (4.2)–(4.4), (4.10)–(4.12), and the triangle inequality, we have
|H3,1(f)|=|d3(d2d4−d23)−d4(d4−d2d3)+d5(d3−d22)|≤|d3||d2d4−d23|+|d4||d4−d2d3|+|d5||d3−d22|≤34171147456, |
which completes the proof.
Theorem 5.1. If f∈H(λ) and is of the form (1.1), then
|a2|≤18λ2−8λ+4, |
|a3|≤110λ2−12λ+6, |
|a3−νa22|≤{ν[3(1−λ)2+2λ2]−2(1−λ)λ16[3(1−λ)2+2λ2][(1−λ)2+λ2]2,ν≥t1,12[3(1−λ)2+2λ2],t2<ν<t1,2(1−λ)λ−ν[3(1−λ)2+2λ2]16[3(1−λ)2+2λ2][(1−λ)2+λ2]2,ν≤t2, | (5.1) |
where
t1=8[(1−λ)2+λ2]2+2λ(1−λ)3(1−λ)2+2λ2,t2=2λ(1−λ)−8[(1−λ)2+λ2]23(1−λ)2+2λ2. |
The result is sharp for the function p(z)=(1+z2)/(1−z2).
Proof.
f′(z)=1+2a2z+3a3z2+4a4z3+5a5z4+⋅⋅⋅, |
(1−λ)(f′(z))1−λ=(1−λ)+2(1−λ)2a2z+(3(1−λ)2a3−2(1−λ)2λa22)z2+⋅⋅⋅, | (5.2) |
2zf′(z)f(z)−f(−z)=1+2a2z+2a3z2+(4a4−2a2a3)z3+⋅⋅⋅, |
λ(2zf′(z)f(z)−f(−z))λ=λ+2λ2a2z+(2λ2a3−2λ2(1−λ)a22)z2+⋅⋅⋅. | (5.3) |
In addition,
(1−λ)(f′(z))1−λ+λ(2zf′(z)f(z)−f(−z))λ=21+e−w(z)=1+c14z+(c24−c218)z2+⋅⋅⋅, | (5.4) |
where
w(z)=p(z)−1p(z)+1=12c1z+(12c2−14c21)z2+(18c31−12c2c1+12c3)z3+⋅⋅⋅. |
p(z)=1+c1z+c2z2+c3z3+⋅⋅⋅∈P. |
Substituting (5.2) and (5.3) into (5.4) and comparing the coefficients on both sides of (5.4), we can obtain
[2(1−λ)2+2λ2]a2=c14, | (5.5) |
[3(1−λ)2+2λ2]a3−[2(1−λ)2λ+2λ2(1−λ)]a22=c24−c218. | (5.6) |
From (5.5) and (5.6), we have
a2=c18[(1−λ)2+λ2], | (5.7) |
a3=13(1−λ)2+2λ2A, | (5.8) |
where
A={(1−λ)λ32[(1−λ)2+λ2]2−18}c21+c24. |
Hence,
|a3|=14[3(1−λ)2+2λ2]|c2−(12−(1−λ)λ8[(1−λ)2+λ2]2)c21|, |
and, since
|2(12−(1−λ)λ8[(1−λ)2+λ2]2)−1|=(1−λ)λ4[(1−λ)2+λ2]2<1λ∈[0,1], |
we can apply Lemma 2.2 to get
|a3|≤110λ2−12λ+6. |
From (5.7) and (5.8), we can get
|a3−νa22|=14[3(1−λ)2+2λ2]|c2−{ν[3(1−λ)2+2λ2]16[(1−λ)2+λ2]2−(1−λ)λ8[(1−λ)2+λ2]2+12}c21|. |
Applying Lemma 2.2, we can obtain
|a3−νa22|≤12[3(1−λ)2+2λ2]max{1,|ν[3(1−λ)2+2λ2]−2(1−λ)λ8[(1−λ)2+λ2]2|}. |
Then, we get (5.1), which completes the proof.
Corollary 5.1. If f∈H(12) and is of the form (1.1), then
|a3−νa22|≤{5ν−220,ν≥2,25,−65<ν<2,2−5ν20,ν≤−65. | (5.9) |
Now, we assume that ψ(z) is an analytic and univalent function with positive real part in D, and ψ(z) satisfies the condition of ψ(0)=1 and ψ′(0)>0. It is easy to know that ψ(z) has a series expansion of the form
ψ(z)=1+A1z+A2z2+A3z3+⋅⋅⋅. |
Next, we are going to estimate the upper bounds of the initial coefficients for f, where f and f−1 belong to H(λ,ψ). Since ψ′(0)>0, we have A1>0.
Remark 6.1. For ψ(z)=√1+z, f(z)=z, we have that f(z) and f−1(z) belong to H(λ,ψ) always holds.
Theorem 6.1. If f, g belong to H(λ,ψ) and are of the form (1.1), where g is the inverse function of f, then we have
|a2|≤min{A12[λ2+(1−λ)2],√A1+|A2−A1|7λ2−8λ+3}, |
|a3|≤min{A12λ2+3(1−λ)2+A214[(1−λ)2+λ2]2,A1+|A2−A1|7λ2−8λ+3}. |
Proof. Since f,g∈H(λ,ψ), there exists two analytic functions u,v:D→D, where u(0)=v(0)=0, such that
(1−λ)(f′(z))1−λ+λ(2zf′(z)f(z)−f(−z))λ=ψ(u(z)), | (6.1) |
(1−λ)(g′(z))1−λ+λ(2zg′(z)g(z)−g(−z))λ=ψ(v(z)). | (6.2) |
Let us define the functions p and q by
p(z)=1+p1z+p2z2+⋅⋅⋅=1+u(z)1−u(z), |
q(z)=1+q1z+q2z2+⋅⋅⋅=1+v(z)1−v(z). |
Or, equivalently,
u(z)=p(z)−1p(z)+1=12p1z+(p22−p214)z2+⋅⋅⋅, |
v(z)=q(z)−1q(z)+1=12q1z+(q22−q214)z2+⋅⋅⋅. |
In addition,
ψ(u(z))=1+12A1p1z+(A1(12p2−14p21)+14A2p21)z2+⋅⋅⋅, | (6.3) |
ψ(v(z))=1+12A1q1z+(A1(12q2−14q21)+14A2q21)z2+⋅⋅⋅. | (6.4) |
From (5.2), (5.3), (6.1), and (6.3), we have
2[λ2+(1−λ)2]a2=12A1p1, | (6.5) |
[3(1−λ)2+2λ2]a3−2λ(1−λ)a22=A1(12p2−14p21)+14A2p21. | (6.6) |
Since
g(z)=z−a2z2+(2a22−a3)z3−(5a32−5a2a3+a4)z4+⋅⋅⋅, |
we can obtain
(1−λ)(g′(z))1−λ+λ(2zg′(z)g(z)−g(−z))λ=1−2[(1−λ)2+λ2]a2z+[(3(1−λ)2+2λ2)(2a22−a3)−2λ(1−λ)a22]z2−⋅⋅⋅. | (6.7) |
By using (6.2), (6.4), and (6.7), we have
−2[(1−λ)2+λ2]a2=12A1q1, | (6.8) |
[3(1−λ)2+2λ2](2a22−a3)−2λ(1−λ)a22=A1(12q2−14q21)+14A2q21. | (6.9) |
From (6.5) and (6.8), we can get
p1=−q1, | (6.10) |
and
a22=A21(p21+q21)32[λ2+(1−λ)2]2. | (6.11) |
Since |pi|≤2,|qi|≤2(i∈N+), we obtain
|a2|≤A12[λ2+(1−λ)2]. | (6.12) |
By adding (6.6) to (6.9), we can get
a22=2A1(p2+q2)+(A2−A1)(p21+q21)8(7λ2−8λ+3). | (6.13) |
Since |pi|≤2and|qi|≤2(i∈N+), we can get
|a2|≤√A1+|A2−A1|7λ2−8λ+3. | (6.14) |
From (6.12) and (6.14), we can obtain the conclusion
|a2|≤min{A12[λ2+(1−λ)2],√A1+|A2−A1|7λ2−8λ+3}. |
By subtracting (6.6) from (6.9) and using (6.10), we have
a3=A1(p2−q2)4[2λ2+3(1−λ)2]2+a22. | (6.15) |
Using (6.10) and (6.11) in (6.15), we can obtain
a3=A1(p2−q2)4[3(1−λ)2+2λ2]+A21p2116[(1−λ)2+λ2]2. |
Therefore,
|a3|≤A12λ2+3(1−λ)2+A214[(1−λ)2+λ2]2. | (6.16) |
On the other hand, by using (6.10) and (6.13) in (6.15), we can obtain
a3=A1(p2−q2)4[3(1−λ)2+2λ2]+A1(p2+q2)+(A2−A1)p214[3(1−λ)2+2λ2]−8λ(1−λ), |
or, equivalently,
a3=(A1p2(14(5λ2−6λ+3)+14(7λ2−8λ+3))+A1q2(14(7λ2−8λ+3)−14(5λ2−6λ+3))+(A2−A1)p214(7λ2−8λ+3)). |
Using the triangle inequality and Lemma 2.2, we can obtain
|a3|≤A17λ2−8λ+3+|A2−A1|7λ2−8λ+3. | (6.17) |
From (6.16) and (6.17), we have
|a3|≤min{A12λ2+3(1−λ)2+A214[(1−λ)2+λ2]2,A1+|A2−A1|7λ2−8λ+3}, |
which completes the proof.
Corollary 6.1. If f satisfies the condition of Theorem 6.1 and we let ψ(z)=1+43z+23z2, then
|a2|≤min{23[λ2+(1−λ)2],√27λ2−8λ+3}, |
|a3|≤min{43[2λ2+3(1−λ)2]+49[(1−λ)2+λ2]2,27λ2−8λ+3}. |
Corollary 6.2. If f satisfies the condition of Theorem 6.1 and we let f∈H(0,ψ), then
|a2|≤min{A12,√A1+|A2−A1|3}, |
|a3|≤min{A13+A214,A1+|A2−A1|3}. |
Let f∈H(1,ψ), then
|a2|≤min{A12,√A1+|A2−A1|2}, |
|a3|≤min{A12+A214,A1+|A2−A1|2}. |
In the present work, we defined new subclasses of analytic functions associated with the modified sigmoid function. Then, we mainly get upper bounds of the third-order Hankel determinant and fourth-order Hankel determinant in certain conditions. We also get the upper bound of the third-order Hankel determinant of its inverse function in the specific conditions mentioned above. Next, we investigated the upper bound of the Fekete-Szegö inequality for the analytic functions in the class H(λ). Finally, we estimated the upper bounds of the initial coefficients for the analytic functions in the class H(λ,ψ), where f−1(z) also belongs to H(λ,ψ). The purpose of our study is to stimulate the interest of scholars in the field and to further stimulate their research in this kind of subject. In fact, this kind of problem plays a very important role in many other problems of mathematical analysis.
We will further investigate the upper bounds of the third, fourth, and fifth-order Hankel determinants of functions belonging to H(λ) or H(λ,ψ) (0≤λ≤1). We can also research the upper bounds of the third or fourth Hankel determinant of a class of functions defined in [12]. Recently, the problems of the quantum calculus happens to provide another popular and interesting direction for researchers in complex analysis, which is evidenced by the recently-published review article by Srivastava [31]. Hence, the quantum extension of the results shown in this paper is quite worthwhile to further research. Apart from the above, we are motivated to explore how to get the upper bound of the Hankel determinant of certain analytic functions by other methods, from which we may get more precise or sharp upper bounds.
The authors declare they have not used Artificial Intelligence (AI) tools in the creation of this article.
This study is supported by the Guangdong Provincial Natural Science Foundation's general program. Fund number: 2021A1515010374.
Also, the authors would like to thank the anonymous referee for the very thorough reading and contributions to improve our presentation of the paper.
The authors declare that they have no competing interests.
[1] | I. Graham, G. Kohr, Geometric function theory in one and higher dimensions, New York: Marcel Dekker, 2003. https://doi.org/10.1201/9780203911624 |
[2] |
J. W. Noonan, D. K. Thomas, On the second Hankel determinant of areally mean p-valent functions, T. Am. Math. Soc., 223 (1976), 337–346. https://doi.org/10.1090/S0002-9947-1976-0422607-9 doi: 10.1090/S0002-9947-1976-0422607-9
![]() |
[3] | W. Ma, C. Minda, Aunified treatment of some special classes of univalent functions, Proceedings of the Conference on Complex Analysis, Boston: International Press, 1992. |
[4] |
P. Goel, S. S. Kumar, Certain class of starlike functions associated with modified function, B. Malays. Math. Sci. So., 43 (2020), 957–991. https://doi.org/10.1007/s40840-019-00784-y doi: 10.1007/s40840-019-00784-y
![]() |
[5] | J. Sokół, J. Stankiewicz, Radius of convexity of some subclasses of strongly starlike functions, Zeszyty Nauk. Politech. Rzeszowskiej Mat., 19 (1996), 101–105. |
[6] |
K. Sharma, N. K. Jain, V. Ravichandran, Starlike functions associated with a cardioid, Afr. Mat., 27 (2016), 923–939. https://doi.org/10.1007/s13370-015-0387-7 doi: 10.1007/s13370-015-0387-7
![]() |
[7] |
L. Shi, I. Ali, M. Arif, N. E. Cho, S. Hussain, H. Khan, A study of third Hankel determinant problem for certain subfamilies of analytic functions involving cardioid domain, Mathematics, 7 (2019), 418. https://doi.org/10.3390/math7050418 doi: 10.3390/math7050418
![]() |
[8] |
R. Mendiratta, S. Nagpal, V. Ravichandran, On a subclass of strongly starlike functions associated with exponential function, B. Malays. Math. Sci. So., 38 (2015), 365–386. https://doi.org/10.1093/oxarti/kcv022 doi: 10.1093/oxarti/kcv022
![]() |
[9] |
R. K. Raina, J. Sokol, On coefficient estimates for a certain class of starlike functions, Hacet. J. Math. Stat., 44 (2015), 1427–1433. https://doi.org/10.15672/HJMS.2015449676 doi: 10.15672/HJMS.2015449676
![]() |
[10] | S. S. Kumar, K. Arora, Starlike functions associated with a petal shaped domain, arXiv Preprint, 2020. |
[11] | A. Alotaibi, M. Arif, M. A. Alghamdi, S. Hussain, Starlikness associated with cosine hyperbolic function, Mathematics, 8 (2020), 1–16. https://doi.org/10.3390/math8071118 |
[12] |
H. Tang, G. Murugusundaramoorthy, S. H. Li, L. N. Ma, Fekete-Szegö and Hankel inequalities for certain class of analytic functions related to the sine function, AIMS Math., 7 (2022), 6365–6380. https://doi.org/10.3934/math.2022354 doi: 10.3934/math.2022354
![]() |
[13] |
R. R. London, Fekete-Szegő inequalities for close-to-convex functions, P. Am. Math. Soc., 117 (1993), 947–950. https://doi.org/10.2307/2159520 doi: 10.2307/2159520
![]() |
[14] |
M. Çağlar, H. Orhan, N. Yağmur, Coefficient bounds for new subclasses of bi-univalent functions, Filomat, 27 (2013), 1165–1171. https://doi.org/10.2298/FIL1307165C doi: 10.2298/FIL1307165C
![]() |
[15] |
M. Arif, K. I. Noor, M. Raza, Hankel determinant problem of a subclass of analytic functions, J. Inequal. Appl., 2012 (2012), 1–7. https://doi.org/10.1186/1029-242X-2012-22 doi: 10.1186/1029-242X-2012-22
![]() |
[16] |
N. E. Cho, B. Kowalczyk, O. S. Kwon, A. Lecko, Some coefficient inequalities related to the Hankel determinant for strongly starlike functions of order alpha, J. Math. Inequal., 11 (2017), 429–439. https://doi.org/10.7153/jmi-2017-11-36 doi: 10.7153/jmi-2017-11-36
![]() |
[17] |
N. E. Cho, V. Kumar, Initial coefficients and fourth Hankel determinant for certain analytic functions, Miskolc Math. Notes, 21 (2020), 763–779. https://doi.org/10.18514/MMN.2020.3083 doi: 10.18514/MMN.2020.3083
![]() |
[18] |
M. G. Khan, N. E. Cho, T. G. Shaba, B. Hhemad, W. K. Mashwani, Coefficient functional for a class of bounded turning functions related to modified sigmoid function, AIMS Math., 7 (2021), 3133–3149. https://doi.org/10.3934/math.2022173 doi: 10.3934/math.2022173
![]() |
[19] |
G. Murugusundaramoorthy, M. G. Khan, B. Ahmad, W. K. Mashwani, Coefficient functionals for a class of bounded turning functions connected to three leaf function, J. Math. Comput. Sci., 28 (2022), 213–223. https://doi.org/10.22436/jmcs.028.03.01 doi: 10.22436/jmcs.028.03.01
![]() |
[20] |
D. Mohamad, N. H. A. A. Wahid, N. N. M. Fauzi, Some properties of a new subclass of tilted star-like functions with respect to symmetric conjugate points, AIMS Math., 8 (2023), 1889–1900. https://doi.org/10.3934/math.2023097 doi: 10.3934/math.2023097
![]() |
[21] |
E. Rodemich, The fifth coefficient for bounded univalent functions with real coefficients, Adv. Math., 263 (2014), 468–512. https://doi.org/10.1016/j.aim.2014.06.012 doi: 10.1016/j.aim.2014.06.012
![]() |
[22] |
E. Haliloglu, On the Faber coefficients of functions univalent in an ellipse, T. Am. Math. Soc., 349 (1997), 2901–2916. https://doi.org/10.1090/S0002-9947-97-01721-2 doi: 10.1090/S0002-9947-97-01721-2
![]() |
[23] |
R. J. Libera, E. J. Złotkiewicz, Early coefficients of the inverse of a regular convex function, P. Am. Math. Soc., 85 (1982), 225–230. https://doi.org/10.1090/S0002-9939-1982-0652447-5 doi: 10.1090/S0002-9939-1982-0652447-5
![]() |
[24] |
T. Panigrahi, B. B. Mishra, A. Naik, Coefficient bounds for the family of bounded turning functions associated with tan hyperbolic function, Palestine J. Math., 12 (2023), 620–634. https://doi.org/10.1007/s11253-023-02177-8 doi: 10.1007/s11253-023-02177-8
![]() |
[25] |
K. I. Noor, N. Khan, Q. Z. Ahmad, Coeffcient bounds for a subclass of multivalent functions of reciprocal order, AIMS Math., 2 (2017), 322–335. https://doi.org/10.3934/Math.2017.2.322 doi: 10.3934/Math.2017.2.322
![]() |
[26] |
B. A. Frasin, M. K. Aouf, New subclasses of bi-univalent functions, Appl. Math. Lett., 24 (2011), 1569–1573. https://doi.org/10.1016/j.aml.2011.03.048 doi: 10.1016/j.aml.2011.03.048
![]() |
[27] |
F. Rønning, Uniformly convex functions and a corresponding class of starlike functions, P. Am. Math. Soc., 118 (1993), 189–196. https://doi.org/10.1090/S0002-9939-1993-1128729-7 doi: 10.1090/S0002-9939-1993-1128729-7
![]() |
[28] |
Y. Li, K. Vijaya, G. Murugusundaramoorthy, H. Tang, On new subclasses of bi-starlike functions with bounded boundary rotation, AIMS Math., 5 (2020), 3346–3356. https://doi.org/10.3934/math.2020215 doi: 10.3934/math.2020215
![]() |
[29] |
P. Zaprawa, On the Fekete-Szegö problem for classes of bi-univalent functions, B. Belg. Math. Soc.-Sim., 21 (2014), 169–178. https://doi.org/10.36045/bbms/1394544302 doi: 10.36045/bbms/1394544302
![]() |
[30] | D. A. Brannan, J. G. Clunie, Aspects of contemporary complex analysis, New York: Academic Press, 1980. |
[31] |
H. M. Srivastava, Operators of basic (or q-) calculus and fractional q-calculus and their applicationsin geometric function theory of complex analysis, Iran. J. Sci. Technol., 44 (2020), 327–344. https://doi.org/10.1007/s40995-019-00815-0 doi: 10.1007/s40995-019-00815-0
![]() |
1. | Huo Tang, Muhammad Abbas, Reem K. Alhefthi, Muhammad Arif, Problems involving combinations of coefficients for the inverse of some complex-valued analytical functions, 2024, 9, 2473-6988, 28931, 10.3934/math.20241404 | |
2. | Timilehin Gideon Shaba, Ferdous M. O. Tawfiq, Daniel Breaz, Luminit̨a-Ioana Cotîrlă, New Uses of q-Generalized Janowski Function in q-Bounded Turning Functions, 2024, 12, 2227-7390, 1552, 10.3390/math12101552 | |
3. | Timilehin Gideon Shaba, Serkan Araci, Babatunde Olufemi Adebesin, Fuat Usta, Bilal Khan, Characterization of Bi-Starlike Functions: A Daehee Polynomial Approach, 2024, 16, 2073-8994, 1640, 10.3390/sym16121640 |