In the current article, we consider a class of bounded turning functions associated with the cosine hyperbolic function and give some results containing coefficient functionals using the familiar Carathéodory functions. An improvement on the bound of the third-order Hankel determinant for functions in this class is provided. Furthermore, we obtain sharp estimates of the Fekete-Szegö, Krushkal, and Zalcman functionals with logarithmic coefficients as entries. All the findings are proved to be sharp.
Citation: 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[J]. AIMS Mathematics, 2024, 9(6): 15761-15781. doi: 10.3934/math.2024761
[1] | 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 |
[2] | Muhammmad Ghaffar Khan, Wali Khan Mashwani, Jong-Suk Ro, Bakhtiar Ahmad . Problems concerning sharp coefficient functionals of bounded turning functions. AIMS Mathematics, 2023, 8(11): 27396-27413. doi: 10.3934/math.20231402 |
[3] | 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 |
[4] | 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 |
[5] | 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 |
[6] | Afis Saliu, Khalida Inayat Noor, Saqib Hussain, Maslina Darus . Some results for the family of univalent functions related with Limaçon domain. AIMS Mathematics, 2021, 6(4): 3410-3431. doi: 10.3934/math.2021204 |
[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] | Ebrahim Analouei Adegani, Davood Alimohammadi, Teodor Bulboacă, Nak Eun Cho, Mahmood Bidkham . On the logarithmic coefficients for some classes defined by subordination. AIMS Mathematics, 2023, 8(9): 21732-21745. doi: 10.3934/math.20231108 |
[9] | 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 |
[10] | Wenzheng Hu, Jian Deng . Hankel determinants, Fekete-Szegö inequality, and estimates of initial coefficients for certain subclasses of analytic functions. AIMS Mathematics, 2024, 9(3): 6445-6467. doi: 10.3934/math.2024314 |
In the current article, we consider a class of bounded turning functions associated with the cosine hyperbolic function and give some results containing coefficient functionals using the familiar Carathéodory functions. An improvement on the bound of the third-order Hankel determinant for functions in this class is provided. Furthermore, we obtain sharp estimates of the Fekete-Szegö, Krushkal, and Zalcman functionals with logarithmic coefficients as entries. All the findings are proved to be sharp.
Complex analysis is one of the major disciplines nowadays due to its numerous applications in mathematical science and other fields. Geometric function theory is an intriguing topic of complex analysis that involves the geometrical characteristics of analytic functions. This area is crucial to applied mathematics, particularly in fields such as engineering, electronics, nonlinear integrable system theory, fluid dynamics, modern mathematical physics, and partial differential equation theory. The key problem that led to the rapid emergence of geometric function theory is the Bieberbach conjecture. It is about the coefficient bounds for functions belonging to the class S of univalent functions. This conjecture states that if g∈S with the Taylor-Maclaurin series expansion of the form
g(z)=z+∞∑k=2dkzk,z∈D, | (1.1) |
where D:={z∈C:|z|<1}, then |dk|≤k for all k≥2. Let A be the class of analytic functions with the series representation given in (1.1). The set S is a subclass of A which was first taken into account by Koebe in 1907. The above famous conjecture was proposed by Bieberbach [1] in 1916. He proved this for k=2, and subsequent researchers, including L öwner [2], Garabedian and Schiffer [3], Pederson and Schiffer [4], and Pederson [5], confirmed it for k=3, 4, 5, and 6, respectively. However, settling the conjecture for k≥7 remained elusive until 1985 when de Branges [6] used hypergeometric functions to prove it for every k≥2. Lawrence Zalcman proposed the inequality |d2k−d2k−1|≤(k−1)2 with k≥2 for g∈S in the late 1960's as a way of establishing the Bieberbach conjecture. Due to this, a number of articles [7,8,9] have been published on the Zalcman hypothesis and its generalized form |λd2k−d2k−1|≤λk2−2k+1 with λ≥0 for different subclasses of the class S. This conjecture has remained unsolved for a long time. Krushkal [10] established this hypothesis for k≤6. In an attempt to solve the Zalcman conjecture, Krushkal [11] investigated the inequality |dlk−dl(k−1)2|≤2l(k−1)−kl with k,l≥2 for g∈S. A broader Zalcman hypothesis for g∈S was proposed by Ma [12] later, in 1999, and is given by
|djdk−dj+k−1|≤(j−1)(k−1),j,k≥2. |
He only proved it for a subclass of S. The challenge is still open for the class S.
Now, we recall the definition of subordination, which actually provides a relationship between analytic functions. We write g1≺g2 to illustrate that g1 is subordinate to g2. It is explained that for two given functions g1,g2∈A, a Schwarz function w exists such that g1(z)=g2(w(z)) for z∈D. Once g2 is univalent in D, then this relation is equivalent to saying that
g1(z)≺g2(z),z∈D |
if and only if
g1(0)=g2(0) and g1(D)⊂g2(D). |
The three classic subclasses of univalent functions are C, S∗ and K, of which their functions are known respectively as convex functions, starlike functions and close-to-convex functions. These classes are defined by
C:={g∈S:(zg′(z))′g′(z)≺1+z1−z,z∈D}, |
S∗:={g∈S:zg′(z)g(z)≺1+z1−z,z∈D}, |
and
K:={g∈S:zg′(z)h(z)≺1+z1−z,z∈D} |
for some h∈S∗. Taking h(z)=z, the class K reduces to the class BT of bounded turning functions. Further, replacing 1+z1−z by some other special functions, various interesting subfamilies of the class S were studied; interested readers may refer to [13,14,15,16,17,18].
The determinant Dλ,n(g), where n,λ∈N={1,2,…}, is known as the Hankel determinant and was presented by Pommerenke [19,20]. It is formed by the coefficients of the function g∈S and is defined by
Dλ,n(g):=|dndn+1…dn+λ−1dn+1dn+2…dn+λ⋮⋮…⋮dn+λ−1dn+λ…dn+2λ−2|. |
Hankel matrices are used in both pure mathematics and technological applications, including the theory of Markov processes, the theory of non-stationary signals in the Hamburger moment problem, and many other topics, see for example [21,22,23,24]. There are relatively few publications on the bounds of the Hankel determinant for functions in the general class S. The best estimate for g∈S was determined by Hayman in [25], which asserted that |D2,n(g)|≤|η|, where η is a constant. Additionally, for g∈S, it was shown in [26] that the second-order Hankel determinant |D2,2(g)|≤η for 0≤η≤11/3. The two determinants D2,1(g) and D2,2(g) have been extensively studied in the literature for various subfamilies of univalent functions. The works [27,28,29,30,31], in which the sharp bounds of the second-order Hankel determinant for some subclasses of S are determined, are particularly noteworthy.
In comparison to the second-order Hankel determinant, the sharp bound of the third-order Hankel determinant D3,1(g) for certain analytic univalent functions is much harder to find. The investigation on D3,1(g) for S was initiated by Babalola [32] in 2010. The exact bounds of this determinant were proved recently for the classes C, S∗, and BT in [33], [34], and [35], respectively. These bounds are given by
|D3,1(g)|≤{4135,forg∈C,49,forg∈S∗,14,forg∈BT. |
By employing similar techniques, Khalil Ullah et al. [36] and Lecko et al. [37] derived the sharp bounds for |D3,1(g)| when considering functions belonging to the families S∗tanh and S∗(1/2), respectively. Additionally, the works [38,39,40,41,42,43] proved the sharp bounds for the same third-order Hankel determinant in various novel subfamilies of analytic univalent functions.
Let us consider the two function classes defined respectively by
S∗cosh:={g∈S:zg′(z)g(z)≺cosh√z (z∈D)} |
and
BTcosh:={g∈S:g′(z)≺cosh√z (z∈D)}. |
These classes were introduced and studied by Mundalia et al. [44] and Ghaffar et al. [45], respectively. In this paper, we improved the bound of the third-order Hankel determinant |D3,1(g)|, which was determined by Ghaffar et al. and published recently in AIMS Mathematics [45]. Furthermore, we obtain the sharp estimates of the Fekete-Szegö, Krushkal, and Zalcman functionals with logarithmic coefficients as entries.
In the theory of univalent functions, the Carathéodory functions are well studied. They are analytic in D with positive real part and take series representations of the form
p(z)=1+∞∑n=1τnzn (z∈D). | (2.1) |
We denote by P the set of these functions.
To prove the main theorems, we need the following lemmas.
Lemma 2.1 [46] Let p∈P be the form of (2.1) with τ1≥0. Then
2τ2=τ21+β(4−τ21), | (2.2) |
4τ3=τ31+2(4−τ21)τ1β−τ1(4−τ21)β2+2(4−τ21)(1−|β|2)η, | (2.3) |
8τ4=τ41+(4−τ21)β[τ21(β2−3β+3)+4β]−4(4−τ21)(1−|β|2)⋅[τ1(β−1)η+¯βη2−(1−|η|2)κ] | (2.4) |
for some β,η,κ∈¯D:={z∈C:|z|≤1}.
Lemma 2.2 [47] If p∈P is of the form (2.1) and ϑ∈C, we have
|τn−ϑτkτn−k|≤2max{1,|2ϑ−1|} | (2.5) |
for all 1≤k≤n−1.
Lemma 2.3 [48] Let μ, λ, ζ, and ς satisfy λ∈(0,1), ζ∈(0,1) and
8λ(1−λ)[(ζς−2μ)2+(ζ(λ+ζ)−ς)2]+ζ(1−ζ)(ς−2λζ)2≤4λζ2(1−ζ)2(1−λ). | (2.6) |
If p∈P is of the form (2.1), then
|μτ41+λτ22+2ζτ1τ3−32ςτ21τ2−τ4|≤2. |
Lemma 2.4 [49] Suppose that p∈P is provided by (2.1). If R∈[0,1] and R(2R−1)≤S≤R, then we have
|τ3−2Rτ1τ2+Sτ31|≤2. | (2.7) |
Theorem 3.1 If g∈BTcosh is of the form (1.1), then
|d5−d2d4|≤110. |
This inequality is sharp.
Proof. Let g∈BTcosh. Then g can be easily expressed by using the Schwarz function as
g′(z)=cosh√w(z), z∈D. |
If p∈P, then we can write it in the form of
p(z)=1+w(z)1−w(z)=1+τ1z+τ2z2+τ3z3+⋯. |
It follows that
w(z)=12τ1z+14(2τ2−τ21)z2+18(τ31−4τ1τ2+4τ3)z3+116(−τ41+6τ21τ2−8τ1τ3−4τ22+8τ4)z4+⋯. | (3.1) |
From (1.1), we have
g′(z)=1+2d2z+3d3z2+4d4z3+5d5z4+⋯. | (3.2) |
Using the series expansion of (3.1) with simple calculation, we get
cosh√w(z)=1+14τ1z+(14τ2−1196τ21)z2+(3015760τ31−1148τ1τ2+14τ3)z3+(14τ4−1196τ22+3011920τ21τ2−15287645120τ41−1148τ1τ3)z4+⋯. | (3.3) |
Comparing the coefficients in (3.2) and (3.3), we obtain
d2=18τ1, | (3.4) |
d3=112τ2−11288τ21, | (3.5) |
d4=30123040τ31+116τ3−11192τ1τ2, | (3.6) |
d5=−11480τ22−152873225600τ41+120τ4+3019600τ21τ2−11240τ1τ3. | (3.7) |
Employing (3.4), (3.6) and (3.7), we may write
|d5−d2d4|=120|13703107520τ41+1124τ22+2(103192)τ1τ3−32(493960)τ21τ2−τ4|.=120|μτ41+λτ22+2ζτ1τ3−32ςτ21τ2−τ4|, | (3.8) |
where
μ=13703107520, λ=1124, ζ=103192, ς=493960. |
These constants satisfy λ∈(0,1), ζ∈(0,1), and
8λ(1−λ)[(ζς−2μ)2+(ζ(λ+ζ)−ς)2]+ζ(1−ζ)(ς−2λζ)2≤4λζ2(1−ζ)2(1−λ). |
Hence, by Lemma 2.3 and (3.8), we deduce that
|d5−d2d4|≤110. |
This required result is sharp and determined by
g4(z)=∫z0(cosh√t4)dt=z+110z5+1216z9+⋯, | (3.9) |
where we choose the branch of the square root function so that
cosh√z4=1+12!z4+14!z8+16!z12+⋯ | (3.10) |
Theorem 3.2 If g∈BTcosh is of the form of (1.1), then
|d5−d23|≤110. |
This inequality is sharp.
Proof. From (3.5) and (3.7), we obtain
|d5−d23|=120|1799331451520τ41+4372τ22+2(1124)τ1τ3−32(32596480)τ21τ2−τ4|=120|μτ41+λτ22+2ζτ1τ3−32ςτ21τ2−τ4|, | (3.11) |
where
μ=1799331451520, λ=4372, ζ=1124, ς=32596480. |
These constants satisfy λ∈(0,1), ζ∈(0,1), and
8λ(1−λ)[(ζς−2μ)2+(ζ(λ+ζ)−ς)2]+ζ(1−ζ)(ς−2λζ)2≤4λζ2(1−ζ)2(1−λ). |
Hence, by Lemma 2.3 and (3.11), we deduce that
|d5−d23|≤110. |
This required outcome is sharp for the function g4 given in (3.9).
Theorem 3.3 If g∈BTcosh is of the form of (1.1), then
|d4−d32|≤18. |
This inequality is sharp.
Proof. Using (3.4) and (3.6), we have
|d4−d32|=116|τ3−2(1124)τ1τ2+(845)τ31|. |
Let R=1124 and S=845. It is clear that
R(2R−1)=−11288≤S≤R. |
All the conditions of Lemma 2.4 are satisfied, and thus we have
|d4−d32|≤18. |
This result is the best possible and equality is attained by
g3(z)=∫z0(cosh√t3)dt=z+18z4+1168z7+⋯, | (3.12) |
where we choose the branch of the square root function so that
cosh√z3=1+12!z3+14!z6+16!z9+⋯ | (3.13) |
Theorem 3.4 If g∈BTcosh is of the form of (1.1), then
|d5−d42|≤110. |
This inequality is sharp.
Proof. From (3.4) and (3.7), we obtain
|d5−d42|=120|32149322560τ41+1124τ22+2(1124)τ1τ3−32(301720)τ21τ2−τ4|=120|μτ41+λτ22+2ζτ1τ3−32ςτ21τ2−τ4|, | (3.14) |
where
μ=32149322560, λ=1124, ζ=1124, ς=301720. |
These constants satisfy λ∈(0,1), ζ∈(0,1), and
8λ(1−λ)[(ζς−2μ)2+(ζ(λ+ζ)−ς)2]+ζ(1−ζ)(ς−2λζ)2≤4λζ2(1−ζ)2(1−λ). |
Hence, by Lemma 2.3 and (3.14), we deduce that
|d5−d42|≤110. |
This required inequality is sharp for the function g4 given in (3.9).
Theorem 3.5 If g∈BTcosh has the form of (1.1), then
|D3,1(g)|≤164. |
This inequality is sharp.
Proof. From the definition, we know
D3,1(g)=2d2d3d4−d33−d24+d3d5−d22d5. | (3.15) |
Let g∈BTcosh and gθ(z)=e−iθg(eiθz) with θ∈R. It is noted that g′θ(z)=g′(eiθz) and thus gθ∈BTcosh for all θ∈R. Since |D3,1(gθ)|=|D3,1(g)|, we may choose the coefficient d2 of g to be a non-negative real number when estimating the functional |D3,1(g)|. Then, since d2=18τ1 and τ1 is a coefficient of a function in P, it follows that τ1 is real and τ1=τ∈[0,2]. Putting the estimations of di's from (3.4), (3.5), (3.6), and (3.7) into D3,1(g) with τ1=τ, we have
D3,1(g)=133443020800(513823τ6−4378896τ4τ2+7922880τ3τ3+5552064τ2τ22−89994240τ2τ4+155312640ττ2τ3−83220480τ32+139345920τ2τ4−130636800τ23). |
Let r=4−τ2. Then, by (2.2), (2.3), and (2.4), we obtain
D3,1(g)=133443020800{−329τ6−10402560β3r3+34836480β3r2+10160640τ3rβ(1−|β|2)η+10160640τ2r¯β(1−|β|2)η2−10160640τ2r(1−|β|2)(1−|η|2)κ+8346240τr2β(1−|β|2)η−2177280τr2β2(1−|β|2)η−34836480r2¯ββη2(1−|β|2)+34836480r2β(1−|β|2)(1−|η|2)κ+2476656τ2r2β2−10160640τ2rβ2−2540160τ4rβ3−12882240τ2r2β3+544320τ2r2β4−32659200r2η2(1−|β|2)2+2555280τ4rβ2+12024τ4rβ−30240τ3r(1−|β|2)η}. |
It is seen that we can write D3,1(g) in the form of
D3,1(g)=133443020800[l1(τ,β)+l2(τ,β)η+l3(τ,β)η2+l4(τ,β,η)κ], |
where β,η,κ∈¯D, and
l1(τ,β)=−329τ6+(4−τ2)[(4−τ2)(−6773760β3−2479680τ2β3+2476656τ2β2+544320τ2β4)+2555280τ4β2+12024τ4β−10160640τ2β2−2540160τ4β3],l2(τ,β)=30240(4−τ2)(1−|β|2)[(4−τ2)(−72τβ2+276τβ)+336τ3β−τ3],l3(τ,β)=725760(4−τ2)(1−|β|2)[(4−τ2)(−3|β|2−45)+14τ2¯β],l4(τ,β,η)=725760(4−τ2)(1−|β|2)(1−|η|2)[48β(4−τ2)−14τ2]. |
By using |β|=ϰ,|η|=y and utilizing the fact |κ|≤1, we obtain
|D3,1(g)|≤133443020800[|l1(τ,β)|+|l2(τ,β)|y+|l3(τ,β)|y2+|l4(τ,β,η)|].≤133443020800M(τ,ϰ,y), | (3.16) |
where
M(τ,ϰ,y)=m1(τ,ϰ)+m2(τ,ϰ)y+m3(τ,ϰ)y2+m4(τ,ϰ)(1−y2), |
with
m1(τ,ϰ)=329τ6+(4−τ2)[(4−τ2)(6773760ϰ3+2479680τ2ϰ3+2476656τ2ϰ2+544320τ2ϰ4)+2555280τ4ϰ2+12024τ4ϰ+10160640τ2ϰ2+2540160τ4ϰ3],m2(τ,ϰ)=30240(4−τ2)(1−ϰ2)[(4−τ2)(72τϰ2+276τϰ)+336τ3ϰ+τ3],m3(τ,ϰ)=725760(4−τ2)(1−ϰ2)[(4−τ2)(3ϰ2+45)+14τ2ϰ],m4(τ,ϰ)=725760(4−τ2)(1−ϰ2)[48ϰ(4−τ2)+14τ2]. |
Now, we have to maximize M in the closed cuboid Υ:=[0,2]×[0,1]×[0,1].
In light of (τ,ϰ)∈[0,2]×[0,1], we observe that
m3(τ,ϰ)≤725760(4−τ2)(1−ϰ2)[(4−τ2)(3ϰ2+45)+14τ2]=:g3(τ,ϰ). | (3.17) |
Taking gi(τ,ϰ)=mi(τ,ϰ) for i=1,2,4 and
G(τ,ϰ,y)=g1(τ,ϰ)+g2(τ,ϰ)y+g3(τ,ϰ)y2+g4(τ,ϰ)(1−y2), | (3.18) |
it is not hard to see that M(τ,ϰ,y)≤G(τ,ϰ,y) in the cuboid Υ. In the following, we aim to find the maximum value of G in Υ.
By partially differentiating G with respect to y, we have
∂G∂y=g2(τ,ϰ)+2[g3(τ,ϰ)−g4(τ,ϰ)]y. | (3.19) |
In view of g2(τ,ϰ)≥0 and
g3(τ,ϰ)−g4(τ,ϰ)=725760(4−τ2)(1−ϰ2)[(3ϰ2−48ϰ+45)(4−τ2)]≥0 | (3.20) |
on [0,2]×[0,1], we have ∂G∂y≥0 for all y∈[0,1]. It follows that
G(τ,ϰ,y)≤G(τ,ϰ,1), | (3.21) |
where
G(τ,ϰ,1)=g1(τ,ϰ)+g2(τ,ϰ)+g3(τ,ϰ)=329τ6+72(4−τ2)[q4(τ)ϰ4+q3(τ)ϰ3+q2(τ)ϰ2+q1(τ)ϰ+q0(τ)]=:Q(τ,ϰ), |
where
q4(τ)=7560(4−τ2)(τ2−4τ−4),q3(τ)=840(τ4−30τ3+52τ2−552τ+448),q2(τ)=84(13τ4−365τ3+6678τ2+1440τ−20160),q1(τ)=τ(167τ3+25200τ2+463680),q0(τ)=420(τ3−744τ2+4320). |
Then the problem reduces to finding the maximum value of Q on [0,2]×[0,1]. By noting that q4(τ)≤0 for all τ∈[0,2], we obtain that
Q(τ,ϰ)≤329τ6+72(4−τ2)[q3(τ)ϰ3+q2(τ)ϰ2+q1(τ)ϰ+q0(τ)]=:W(τ,ϰ). | (3.22) |
Setting τ=0, we obtain
W(0,ϰ)=108380160ϰ3−487710720ϰ2+522547200=108380160ϰ2(ϰ−92)+522547200≤522547200≈5.2255×108 |
for all ϰ∈[0,1]. Setting τ=2, we get
W(2,ϰ)≡21056,ϰ∈[0,1]. |
It is left to consider the case of τ∈(0,2). For the system of equations
∂W∂τ=0 and ∂W∂ϰ=0 |
with (τ,ϰ)∈(0,2)×(0,1), a numerical computation indicates that all the real approximate solutions are listed as (1.6125,−1.0547), (158.7578,−0.6573), (2.0982,−0.4927), (2.1274,0.3361), (1.0709,0.9834), (0,0), and (2,2.1500). Thus, the only critical point of W that lies in (0,2)×(0,1) is about (1.0709,0.9834). For this point, we have W(1.0709,0.9834)≈1.9621×108.
Thus, from above cases, we conclude that
M(τ,ϰ,y)≤G(τ,ϰ,y)≤G(τ,ϰ,1)≤Q(τ,ϰ)≤W(τ,ϰ)≤522547200 |
on [0,2]×[0,1]×[0,1]. From (3.16) we get that
|D3,1(g)|≤133443020800[M(τ,ϰ,y)]≤52254720033443020800=164. |
If g∈BTcosh, then the sharp bound for this Hankel determinant is determined by
|D3,1(g)|=164≈0.01562, |
with an extremal function g3 given in (3.12).
The logarithmic coefficients ξk of g∈S are given by
Gg(z):=log(g(z)z)=2∞∑k=1ξkzk,z∈D. |
These coefficients contribute significantly in many estimations to the theory of univalent functions. In 1985, de Branges [6] completed the proof of the Milin conjecture [50], which asserted that for all positive integers k≥1,
k∑l=1l(k−l+1)|ξk|2≤k∑l=1k−l+1l, |
and equality holds if and only if g takes the form z/(1−eiφz)2 for some φ∈R. This inequality leads to the famous Bieberbach–Robertson–Milin conjectures. In 2005, Kayumov [51] was able to solve the Brennans conjecture for conformal mappings by considering the logarithmic coefficients. For some recent works on the study of logarithmic coefficients, see, for example, [52,53,54,55,56].
If g∈S is in the form of (1.1), then its logarithmic coefficients are given by
ξ1=12d2, | (4.1) |
ξ2=12(d3−12d22), | (4.2) |
ξ3=12(d4−d2d3+13d32), | (4.3) |
ξ4=12(d5−d2d4+d22d3−12d23−14d42). | (4.4) |
Plugging (3.4), (3.5), (3.6), and (3.7) into (4.1), (4.2), (4.3), and (4.4), we get
ξ1=116τ1, | (4.5) |
ξ2=124τ2−532304τ21, | (4.6) |
ξ3=717680τ31+132τ3−13384τ1τ2, | (4.7) |
ξ4=−191440τ22−1802099464486400τ41+140τ4+14861691200τ21τ2−1033840τ1τ3. | (4.8) |
Define
D2,1(Gg/2):=ξ1ξ3−ξ22, | (4.9) |
D2,2(Gg/2):=ξ2ξ4−ξ23. | (4.10) |
It is observed that D2,1(Gg/2) resembles the well-known functional D2,1(g)=d1d3−d22 over the class S or its subclasses.
Theorem 4.1 If g∈BTcosh is of the form (1.1), then
|ξ2−ϑξ21|≤max{112,|9ϑ+5|576},ϑ∈C. |
This inequality is sharp.
Proof. By employing (4.5) and (4.6), we may write
|ξ2−ϑξ21|=124|τ2−9ϑ+5396τ21|. |
An application of Lemma 2.2 leads to
|ξ2−ϑξ21|≤max{112,|9ϑ+5|576}. |
The bound 112 is achieved by the function g2 given as
g2(z)=∫z0(cosh√t2)dt=z+16z3+1120z5+⋯. | (4.11) |
The bound |9ϑ+5|576 for ϑ∈C is attained by the function g1 given as
g1(z)=∫z0(cosh√t)dt=z+14z2+172z3+⋯. | (4.12) |
Here, we choose the branch of the square root function so that
cosh√z2=1+12!z2+14!z4+16!z6+⋯ | (4.13) |
and
cosh√z=1+12!z+14!z2+16!z3+⋯. | (4.14) |
Substituting ϑ=1, we deduce the corollary stated below.
Corollary 4.1 If the function g∈BTcosh has the form of (1.1), then
|ξ2−ξ21|≤112. |
This bound is achieved by the function g2 given in (4.11).
Theorem 4.2 If g∈BTcosh has the form of (1.1), then
|ξ1ξ2−ξ3|≤116. |
This inequality is sharp.
Proof. Using (4.5), (4.6), and (4.7), we have
|ξ1ξ2−ξ3|=132|τ3−2(712)τ1τ2+19695760τ31|. |
Let R=712 and S=19695760. It is clear that
R(2R−1)=772≤S≤R. |
By Lemma 2.4, we obtain
|ξ1ξ2−ξ3|≤116. |
The equality is attained by the function g3 given in (3.12).
Theorem 4.3 Let g∈BTcosh have the series expansion (1.1). Then
|ξ4−ξ1ξ3|≤120. |
The inequality is sharp.
Proof. From (4.5), (4.7), and (4.8), we have
|ξ4−ξ1ξ3|=140|207047911612160τ41+1936τ22+2(221384)τ1τ3−32(3264751840)τ21τ2−τ4|=140|μτ41+λτ22+2ζτ1τ3−32ςτ21τ2−τ4|, | (4.15) |
where
μ=207047911612160, λ=1936, ζ=221384, ς=3264751840. |
These constants satisfy λ∈(0,1), ζ∈(0,1), and
8λ(1−λ)[(ζς−2μ)2+(ζ(λ+ζ)−ς)2]+ζ(1−ζ)(ς−2λζ)2≤4λζ2(1−ζ)2(1−λ). |
Hence, by Lemma 2.3 and (4.15), we deduce that
|ξ4−ξ1ξ3|≤120. |
This equality is achieved by the function g4 given in (3.9).
Theorem 4.4 Let g∈BTcosh be in the form of (1.1). Then
|ξ4−ξ22|≤120. |
This inequality is sharp.
Proof. From (4.6) and (4.8), we obtain
|ξ4−ξ22|=140|409577323224320τ41+4372τ22+2(103192)τ1τ3−32(809312960)τ21τ2−τ4|.=140|μτ41+λτ22+2ζτ1τ3−32ςτ21τ2−τ4|, | (4.16) |
where
μ=409577323224320, λ=4372, ζ=103192, ς=809312960. |
These constants satisfy λ∈(0,1), ζ∈(0,1), and
8λ(1−λ)[(ζς−2μ)2+(ζ(λ+ζ)−ς)2]+ζ(1−ζ)(ς−2λζ)2≤4λζ2(1−ζ)2(1−λ). |
Hence, by Lemma 2.3 and (4.16), we deduce that
|ξ4−ξ22|≤120. |
The required inequality is sharp and determined by the function g4 given in (3.9).
Theorem 4.5 If g∈BTcosh has the form of (1.1), then
|ξ3−ξ31|≤116. |
This inequality is sharp.
Proof. Using (4.5) and (4.7), we have
|ξ3−ξ31|=132|τ3−2(1324)τ1τ2+5531920τ31|. |
Let R=1324 and S=5531920. It is clear that
R(2R−1)=13288≤S≤R. |
By Lemma 2.4, it follows that
|ξ3−ξ31|≤116. |
This result is the best possible and the extremal function is g3 as given in (3.12).
Theorem 4.6 If g∈BTcosh is of the form (1.1), then
|ξ4−ξ41|≤120. |
This inequality is sharp.
Proof. From (4.5) and (4.8), we obtain
|ξ4−ξ41|=140|361837323224320τ41+1936τ22+2(103192)τ1τ3−32(1486125920)τ21τ2−τ4|.=140|μτ41+λτ22+2ζτ1τ3−32ςτ21τ2−τ4|, | (4.17) |
where
μ=361837323224320, λ=1936, ζ=103192, ς=1486125920. |
These constants satisfy λ∈(0,1), ζ∈(0,1), and
8λ(1−λ)[(ζς−2μ)2+(ζ(λ+ζ)−ς)2]+ζ(1−ζ)(ς−2λζ)2≤4λζ2(1−ζ)2(1−λ). |
Hence, by Lemma 2.3 and (4.17), we deduce that
|ξ4−ξ41|≤120. |
This required inequality is sharp and determined by using (4.1), (4.4) and (3.9).
Theorem 4.7 If g∈BTcosh has the form of (1.1), then
|D2,2(Gg/2)|≤1256. |
This inequality is sharp.
Proof. Suppose that g∈BTcosh and gθ(z)=e−iθg(eiθz) with θ∈R. Since |D2,2(Ggθ/2)|=|D2,2(Gg/2)| for all θ∈R, we still assume that τ1=τ∈[0,2]. Putting (4.6), (4.7), and (4.8) into (4.10) with τ1=τ, we obtain
D2,2(Gg/2)=11070176665600(4047343τ6−32414400τ4τ2+41973120τ3τ3+56996352τ2τ22−615444480τ2τ4+1068318720ττ2τ3−588349440τ32+1114767360τ2τ4−1045094400τ23). |
Let r=4−τ2. Then, by (2.2), (2.3), and (2.4), we obtain
D2,2(Gg/2)=11070176665600{−2237760τ3r(1−|β|2)η−73543680β3r3+278691840β3r2+29030400τ3rβ(1−|β|2)η+29030400τ2r¯βη2(1−|β|2)−29030400τ2r(1−|β|2)(1−|η|2)κ+23224320τβr2η(1−|β|2)−17418240τβ2r2(1−|β|2)η−278691840βr2(1−|β|2)¯βη2+278691840βr2(1−|β|2)(1−|η|2)κ−261273600r2(1−|β|2)2κ2+8376480τ4rβ2−107424τ4βr+8443008τ2β2r2−29030400rτ2β2−7257600τ4rβ3−81285120β3r2τ2+4354560β4r2τ2+2671τ6}. |
It is observed that we can write D2,2(Gg/2) in the form of
D2,2(Gg/2)=11070176665600[k1(τ,β)+k2(τ,β)η+k3(τ,β)η2+k4(τ,β,η)κ], |
where β,η,κ∈¯D, and
k1(τ,β)=2671τ6+(4−τ2)[(4−τ2)(8443008τ2β2−15482880β3−7741440τ2β3+4354560τ2β4)−29030400τ2β2+8376480τ4β2−107424τ4β−7257600τ4β3],k2(τ,β)=60480(4−τ2)(1−|β|2)[(4−τ2)(−288τβ2+384τβ)+480τ3β−37τ3],k3(τ,β)=5806080(4−τ2)(1−|β|2)[(4−τ2)(−3|β|2−45)+5τ2¯β],k4(τ,β,η)=5806080(4−τ2)(1−|β|2)(1−|η|2)[−5τ2+48β(4−τ2)]. |
Now, by using |β|=ϰ,|η|=y and utilizing the fact |κ|≤1, we get
|D2,2(Gg/2)|≤11070176665600[|k1(τ,β)|+|k2(τ,β)|y+|k3(τ,β)|y2+|k4(τ,β,η)|].≤11070176665600Λ(τ,ϰ,y), | (4.18) |
where
Λ(τ,ϰ,y)=t1(τ,ϰ)+t2(τ,ϰ)y+t3(τ,ϰ)y2+t4(τ,ϰ)(1−y2), |
with
t1(τ,ϰ)=2671τ6+(4−τ2)[(4−τ2)(8443008τ2ϰ2+15482880ϰ3+7741440τ2ϰ3+4354560τ2ϰ4)+29030400τ2ϰ2+8376480τ4ϰ2+107424τ4ϰ+7257600τ4ϰ3],t2(τ,ϰ)=60480(4−τ2)(1−ϰ2)[(4−τ2)(288τϰ2+384τϰ)+480τ3ϰ+37τ3],t3(τ,ϰ)=5806080(4−τ2)(1−ϰ2)[(4−τ2)(3ϰ2+45)+5τ2ϰ],t4(τ,ϰ)=5806080(4−τ2)(1−ϰ2)[5τ2+48ϰ(4−τ2)]. |
Now, we have to maximize Λ in the closed cuboid Υ.
In view of
t3(τ,ϰ)≤5806080(4−τ2)(1−ϰ2)[(4−τ2)(3ϰ2+45)+5τ2]=:u3(τ,ϰ) | (4.19) |
for all (τ,ϰ)∈[0,2]×[0,1], by setting ui(τ,ϰ)=ti(τ,ϰ)(i=1,2,4) and
Θ(τ,ϰ,y)=u1(τ,ϰ)+u2(τ,ϰ)y+u3(τ,ϰ)y2+u4(τ,ϰ)(1−y2), |
it is not hard to see that Λ(τ,ϰ,y)≤Θ(τ,ϰ,y) on Υ. In the following, we aim to discuss the maximum value of Θ on Υ.
By partially differentiating Θ with respect to y, we get
∂Θ∂y=u2(τ,ϰ)+2[u3(τ,ϰ)−u4(τ,ϰ)]y. |
Because u2(τ,ϰ)≥0 and
u3(τ,ϰ)−u4(τ,ϰ)=5806080(4−τ2)(1−ϰ2)[(3ϰ2−48ϰ+45)(4−τ2)]≥0 |
on [0,2]×[0,1], we have ∂Θ∂y≥0 for all y∈[0,1]. Hence, we obtain
Θ(τ,ϰ,y)≤Θ(τ,ϰ,1), | (4.20) |
where
Θ(τ,ϰ,1)=u1(τ,ϰ)+u2(τ,ϰ)+u3(τ,ϰ)=2671τ6+288(4−τ2)[v4(τ)ϰ4+v3(τ)ϰ3+v2(τ)ϰ2+v1(τ)ϰ+v0(τ)]=:V(τ,ϰ), |
where
v4(τ)=15120(4−τ2)(τ2−4τ−4), | (4.21) |
v3(τ)=−1680(τ4+12τ3−32τ2+192τ−128), | (4.22) |
v2(τ)=−21(11τ4+3250τ3−45904τ2−11520τ+161280), | (4.23) |
v1(τ)=τ(373τ3+20160τ2+322560), | (4.24) |
v0(τ)=30(259τ3−26880τ2+120960). | (4.25) |
Taking the fact of v4(τ)≤0 for all τ∈[0,2], we obtain
V(τ,ϰ)≤2671τ6+288(4−τ2)[v3(τ)ϰ3+v2(τ)ϰ2+v1(τ)ϰ+v0(τ)]=:K(τ,ϰ). | (4.26) |
Now, we need to find the maximum value of K on [0,2]×[0,1]. For τ=0, we have
K(0,ϰ)=247726080ϰ2(ϰ−634)+4180377600≤4180377600 | (4.27) |
for all ϰ∈[0,1]. If τ=2, it is calculated that K(2,ϰ)≡170944 with ϰ∈[0,1]. Hence, it is left to discuss the case of (τ,ϰ)∈(0,2)×(0,1).
For the system of equations
∂K∂τ=0 and ∂K∂ϰ=0 |
with (τ,ϰ)∈(0,2)×(0,1), a numerical computation indicates that the approximate solutions are (0,0), (1.7758,−1.2237), (2.0405,−0.4933), (52.7638,0.2085), (−212.4757,0.2665), (−2.0293,0.3246), (−1.5447,1.0839), (5.1393,2.5129), (2,2.1720), and (−2,−1.1906). It is found that there are no critical points of K that lie in (0,2)×(0,1).
From the above cases we conclude that
Λ(τ,ϰ,y)≤Θ(τ,ϰ,y)≤Θ(τ,ϰ,1)=V(τ,ϰ)≤K(τ,ϰ)≤4180377600 |
on [0,2]×[0,1]×[0,1]. Using (4.18), we have
|D2,2(Gg/2)|≤11070176665600Λ(τ,ϰ,y)≤41803776001070176665600=1256≈0.003906. |
If g∈BTcosh, then the sharp bound for this second-order Hankel determinant is determined by using (4.2), (4.3), (4.4), and (3.12).
The authors declare that they have not used Artificial Intelligence tools in the creation of this article.
The authors would like to extend their sincere-appreciation to the Researchers Supporting Project number (RSPD2024R802) King Saud University, Riyadh, Saudi Arabia.
Prof. Dr. Nak Eun Cho is the Guest Editor of special issue “Geometric Function Theory and Special Functions” for AIMS Mathematics. Prof. Dr. Nak Eun Cho was not involved in the editorial review and the decision to publish this article.
The authors declare that they have no conflicts of interest.
[1] | L. Bieberbach, Über die Koeffizienten derjenigen Potenzreihen, welche eine schlichte Abbildung des Eintheitskreises vermiteln, Sitzungsberichte Preussische Akademie der Wissenschaften, 138 (1916), 940–955. |
[2] | K. Löwner, Untersuchungen iiber schlichte konforme Abbildungen des Einheitskreises, Math. Ann., 89 (1923), 103–121. |
[3] | P. R. Garabedian, M. Schiffer, A proof of the Bieberbach conjecture for the fourth coefficient, J. Ration. Mech. Anal., 4 (1955), 427–465. |
[4] | R. N. Pederson, M. Schiffer, A proof of the Bieberbach conjecture for the fifth coefficient, Arch. Ration. Mech. Anal., 45 (1972), 161–193. |
[5] | R. N. Pederson, A proof of the Bieberbach conjecture for the sixth coefficient, Arch. Ration. Mech. Anal. 31 (1968), 331–351. |
[6] | L. De Branges, A proof of the Bieberbach conjecture, Acta Math., 154 (1985), 137–152. |
[7] | J. E. Brown, A. Tsao, On the Zalcman conjecture for starlike and typically real functions, Math. Z., 191 (1986), 467–474. |
[8] | L. Li, S. Ponnusamy, J. Qiao, Generalized Zalcman conjecture for convex functions of order α, Acta Math. Hung., 150 (2016), 234–246. |
[9] | W. C. Ma, The Zalcman conjecture for close-to-convex functions, Proc. Amer. Math. Soc., 104 (1988), 741–744. |
[10] | S. L. Krushkal, Proof of the Zalcman conjecture for initial coefficients, Georgian Math. J., 17 (2010), 663–681. |
[11] | S. L. Krushkal, A short geometric proof of the Zalcman and Bieberbach conjectures, 2014. https://doi.org/10.48550/arXiv.1408.1948 |
[12] | W. Ma, Generalized Zalcman conjecture for starlike and typically real functions, J. Math. Anal. Appl., 234 (1999), 328–339. |
[13] | R. Mendiratta, S. Nagpal, V. Ravichandran, On a subclass of strongly starlike functions associated with exponential function, Bull. Malays. Math. Sci. Soc., 38 (2015), 365–386. |
[14] | R. K. Raina, P. Sharma, J. Sokół, Certain classes of analytic functions related to the crescent-shaped regions, J. Contemp. Math. Anal., 53 (2018), 355–362. |
[15] |
L. A. Wani, A. Swaminathan, Radius problems for functions associated with a nephroid domain, RACSAM, 114 (2020), 178. https://doi.org/10.1007/s13398-020-00913-4 doi: 10.1007/s13398-020-00913-4
![]() |
[16] | P. Goel, S. S. Kumar, Certain class of starlike functions associated with modified sigmoid function, Bull. Malays. Math. Sci. Soc., 43 (2020), 957–991. |
[17] | K. Ullah, H. M. Srivastava, A. Rafiq, M. Darus, M. Shutaywi, Radius problems for starlike functions associated with the tan hyperbolic function, J. Funct. Space., 2021 (2021), 9967640. |
[18] | S. Gandhi, P. Gupta, S. Nagpal, V. Ravichandran, Starlike functions associated with an Epicycloid, Hacet. J. Math. Stat., 51 (2022), 1637–1660. |
[19] | C. Pommerenke, On the coefficients and Hankel determinants of univalent functions, J. London Math. Soc., 1 (1966), 111–122. |
[20] | C. Pommerenke, On the Hankel determinants of univalent functions, Mathematika, 14 (1967), 108–112. |
[21] | P. Dienes, The Taylor series: An introduction to the theory of functions of a complex variable, New York: Dover, 1957. |
[22] | D. G. Cantor, Power series with integral coefficients, Bull. Am. Math. Soc., 69 (1963), 362–366. |
[23] | M. A. Hasan, A. A. Hasan, Hankel matrices of finite rank with applications to signal processing and polynomials, J. Math. Anal. Appl., 208 (1997), 218–242. |
[24] | R. Wilson, Determinantal criteria for meromorphic functions, Proc. Lond. Math. Soc., 4 (1954), 357–374. |
[25] | W. K. Hayman, On second Hankel determinant of mean univalent functions, Proc. London Math. Soc., 3 (1968), 77–94. |
[26] | M. Obradović, N. Tuneski, Hankel determinants of second and third order for the class S of univalent functions, Math. Slovaca, 71 (2021), 649–654. |
[27] | A. Janteng, S. A. Halim, M. Darus, Hankel determinant for starlike and convex functions, Int. J. Math. Anal., 1 (2007), 619–625. |
[28] |
S. K. Lee, V. Ravichandran, S. Supramaniam, Bounds for the second Hankel determinant of certain univalent functions, J. Inequal. Appl., 2013 (2013), 281. https://doi.org/10.1186/1029-242X-2013-281 doi: 10.1186/1029-242X-2013-281
![]() |
[29] |
A. Ebadian, T. Bulboacǎ, N. E. Cho, E. A. Adegani, Coefficient bounds and differential subordinations for analytic functions associated with starlike functions, RACSAM, 114 (2020), 128. https://doi.org/10.1007/s13398-020-00871-x doi: 10.1007/s13398-020-00871-x
![]() |
[30] | N. E. Cho, B. Kowalczyk, O. S. Kwon, A. Lecko, Y. J. Sim, The bound of the Hankel detrminant for strongly starlike functions of order alpha, J. Math. Ineq., 11 (2017), 429–439. |
[31] | Y. J. Sim, D. K. Thomas, P. Zaprawa, The second Hankel determinant for starlike and convex functions of order alpha, Complex Var. Elliptic Equations, 67 (2022), 2423–2443. |
[32] | K. O. Babalola, On H3(1) Hankel determinant for some classes of univalent functions, Inequality Theory Appl., 6 (2010), 1–7. |
[33] | B. Kowalczyk, A. Lecko, Y. J. Sim, The sharp bound for the Hankel determinant of the third kind for convex functions, Bull. Aust. Math. Soc., 97 (2018), 435–445. |
[34] | B. Kowalczyk, A. Lecko, D. K. Thomas, The sharp bound of the third Hankel determinant for starlike functions, Forum Math., 34 (2022), 1249–1254. |
[35] |
B. Kowalczyk, A. Lecko, The sharp bound of the third Hankel determinant for functions of bounded turning, Bol. Soc. Mat. Mex., 27 (2021), 69. https://doi.org/10.1007/s40590-021-00383-7 doi: 10.1007/s40590-021-00383-7
![]() |
[36] | K. Ullah, H. M. Srivastava, A. Rafiq, M. Arif, S. Arjika, A study of sharp coefficient bounds for a new subfamily of starlike functions, J. Inequal. Appl., 2021 (2021), 194. |
[37] |
A. Lecko, Y. J. Sim, B. Śmiarowska, The sharp bound of the Hankel determinant of the third kind for starlike functions of order 1/2, Complex Anal. Oper. Theory, 13 (2019), 2231–2238. https://doi.org/10.1007/s11785-018-0819-0 doi: 10.1007/s11785-018-0819-0
![]() |
[38] | M. Arif, O. M. Barukab, S. A. Khan, M. Abbas, The sharp bounds of Hankel Determinants for the families of three-leaf-type analytic functions, Fractal Fract., 6 (2022), 291. |
[39] | O. M. Barukab, M. Arif, M. Abbas, S. A. Khan, Sharp bounds of the coefficient results for the family of bounded turning functions associated with petal shaped domain, J. Funct. Space., 2021 (2021), 5535629. |
[40] | Z. G. Wang, M. Raza, M. Arif, K. Ahmad, On the third and fourth Hankel determinants for a subclass of analytic functions, Bull. Malays. Math. Sci. Soc., 45 (2022), 323–359. |
[41] | B, Kowalczyk, A. Lecko, D. K. Thomas, The sharp bound of the third Hankel determinant of convex functions of order -1/2, J. Math. Inequa., 17 (2023), 191–204. |
[42] | L. Shi, M. Arif, Sharp bounds on the third Hankel determinant for the Ozaki close-to-convex and convex functions, Lith. Math. J., 63 (2023), 487–504. |
[43] | S. Banga, S. S. Kumar, The sharp bounds of the second and third Hankel determinants for the class SL, Math. Slovaca, 70 (2020), 849–862. |
[44] | M. Mundula, S. S. Kumar, On subfamily of starlike functions related to hyperbolic cosine function, J. Anal., 31 (2023), 2043–2062. |
[45] |
M. G. Khan, W. K. Mashwani, L. Shi, S. Araci, B. Ahmad, B. Khan, Hankel inequalities for bounded turning functions in the domain of cosine hyperbolic function, AIMS Mathematics, 8 (2023), 21993–22008. http://doi.org/10.3934/math.20231121 doi: 10.3934/math.20231121
![]() |
[46] | O. S. Kwon, A. Lecko, Y. J. Sim, On the fourth coefficient of functions in the Carathéodory class, Comput. Methods Funct. Theory, 18 (2018), 307–314. |
[47] | I. Efraimidis, A generalization of Livingston's coefficient inequalities for functions with positive real part, J. Math. Anal. Appl., 435 (2016), 369–379. |
[48] | V. Ravichandran, S. Verma, Bound for the fifth coefficient of certain starlike functions, C. R. Math. Acad. Sci. Paris, 353 (2015), 505–510. |
[49] | R. J. Libera, E. J. Zlotkiewicz, Coefficient bounds for the inverse of a function with derivatives in P, Proc. Am. Math. Soc., 87 (1983), 251–257. |
[50] | I. M. Milin, Univalent Functions and Orthonormal Systems (Nauka, Moscow 1971), English Translation, Providence: American Mathematical Society, 1977. |
[51] | I. P. Kayumov, On Brennan's conjecture for a special class of functions, Math. Notes, 78 (2005), 498–502. |
[52] | P. Sunthrayuth, I. Aldawish, M. Arif, M. Abbas, S. El-Deeb, Estimation of the second-order Hankel determinant of logarithmic coefficients for two subclasses of starlike functions, Symmetry, 14 (2022), 2039. |
[53] | Z. Ye, The logarithmic coefficients of close-to-convex functions, Bull. Inst. Math. Acad. Sin.(NS), 3 (2008), 445–452. |
[54] | D. Girela, Logarithmic coefficients of univalent functions, Ann. Acad. Sci. Fenn., 25 (2000), 337–350. |
[55] | L. Shi, M. Arif, A. Rafiq, M. Abbas, J. Iqbal, Sharp Bounds of Hankel Determinant on Logarithmic Coefficients for Functions of Bounded Turning Associated with Petal-Shaped Domain, Mathematics, 10 (2022), 1939. |
[56] | O. Roth, A sharp inequality for the logarithmic coefficients of univalent functions, Proc. Am. Math. Soc., 135 (2007), 2051–2054. |
1. | Muhammad Abbas, Teodor Bulboacă, Reem K. Alhefthi, Muhammad Arif, Third-order Hankel determinant sharp estimates for the inverse of complex valued holomorphic functions, 2025, 11, 24058440, e41666, 10.1016/j.heliyon.2025.e41666 |