Abstract
In this paper, we determine the sharp estimates for Toeplitz determinants of a subclass of close-to-convex harmonic mappings. Moreover, we obtain an improved version of Bohr’s inequalities for a subclass of close-to-convex harmonic mappings, whose analytic parts are Ma-Minda convex functions.
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1 Introduction
A complex-valued function f in the unit disk \(\mathbb {D}=\{z:|z|<1\}\) is called a harmonic mapping if \(\Delta f=4 f_{z \overline{z}}=0\). Let \(\mathcal {H}\) denote the class of sense-preserving harmonic mappings \(f=h +\overline{g}\) in \(\mathbb {D}\), where
are analytic functions in \(\mathbb {D}\). Let \(\mathcal {S}_{\mathcal {H}}\) be the subclass of \(\mathcal {H}\) consisting of univalent mappings. We observe that \(\mathcal {S}_\mathcal {H}\) reduces to the class \(\mathcal {S}\) of normalized univalent analytic functions, if the co-analytic part \(g\equiv 0\). Denote by \(\mathcal {K}_{\mathcal {H}}\) the close-to-convex subclass of \(\mathcal {S}_{\mathcal {H}}\). If \(b_1 = 0\), then the class \(\mathcal {K}_{\mathcal {H}}\) reduces to \(\mathcal {K}^{0}_{\mathcal {H}}\).
Lewy [37] proved that \(f=h+\overline{g}\) is locally univalent in \(\mathbb {D}\) if and only if the Jacobian \(J_{f}=\left| h^{\prime }\right| ^{2}-\left| g^{\prime }\right| ^{2}\ne 0\) in \(\mathbb {D}\). Noting that the harmonic mapping f is sense-preserving, i.e. \(J_{f}>0\) or \(\left| h^{\prime }\right| >\left| g^{\prime }\right| \) in \(\mathbb {D}\). At this point, its dilatation \(\omega _{f}=g^{\prime } / h^{\prime }\) has the property \(\left| \omega _{f}\right| <1\) in \(\mathbb {D}\). The reader can find much information about planar harmonic mappings from [18, 22, 46].
Let \(\mathcal {P}\) denote the class of analytic functions p in \(\mathbb {D}\) of the form
such that \({\text {Re}} (p(z))>0\) in \(\mathbb {D} .\)
Denote by \(\mathcal {A}\) the class of analytic functions in \(\mathbb {D}\) with \(f(0)=f'(0)-1=0\), and \(\mathcal {K}(\alpha )\) denotes the class of functions \(f \in \mathcal {A}\) such that
Particularly, the elements in \(\mathcal {K}(-1 / 2)\) are close-to-convex but are not necessarily starlike in \(\mathbb {D}\). For \(0 \le \alpha <1\), the elements in \(\mathcal {K}(\alpha )\) are known to be convex functions of order \(\alpha \) in \(\mathbb {D}\). For more properties of starlike and convex functions, the reader can refer to the monographs [23, 53].
By making use of the subordination in analytic functions, Ma and Minda [42] introduced a more general class \(\mathcal {C}(\phi )\), consisting of functions in \(\mathcal {S}\) for which
Here the function \(\phi :\mathbb {D} \rightarrow \mathbb {C}\), called Ma-Minda function, is analytic and univalent in \(\mathbb {D}\) such that \(\phi (\mathbb {D})\) has positive real part, symmetric with respect to the real axis, starlike with respect to \(\phi (0)=1\) and \(\phi '(0)>0\) (for more details, see [50, 57]). A Ma-Minda function has the form
The extremal function K for the class \(\mathcal {C}(\phi )\) is given by
which satisfies the condition
We recall the following natural class of close-to-convex harmonic mappings \(\mathcal {M}(\alpha ,\zeta ,n)\), due to Wang et al. [56] (see also [47, 55]).
Definition 1.1
A harmonic mapping \(f=h+\overline{g}\in \mathcal {H}\) is said to be in the class \(\mathcal {M}(\alpha ,\zeta ,n)\) if \(h \in \mathcal {K}(\alpha )\), for some \(\alpha \in \left[ -{1}/{2},1\right) \), given by (1.3) and g satisfies the condition
For \(n=1\), \(\alpha =-{1}/{2}\) and \(|\zeta |=1\), the class \(\mathcal {M}(-{1}/{2},\zeta ,1)\) was introduced by Bharanedhar and Ponnusamy [12]. For \(n=1\), the class \(\mathcal {M}(\alpha ,\zeta ,1)\) was studied in [9, 52].
In 2021, Allu and Halder [9] introduced and investigated the following subclass \(\mathcal {H C}(\phi )\) of close-to-convex harmonic mappings.
Definition 1.2
For \(\zeta \in \mathbb {C}\) with \(|\zeta | \le 1\), let \(\mathcal {H C}(\phi )\) denote the class of harmonic mappings \(f=h+\overline{g}\) in \(\mathbb {D}\) of the form (1.1), whose analytic part h belongs to \(\mathcal {C}(\phi )\) and \(h^{\prime }(0) \ne 0\), along with the condition \(g^{\prime }(z)=\zeta z h^{\prime }(z)\).
Motivated essentially by the classes \(\mathcal {M}(\alpha ,\zeta ,n)\) and \(\mathcal {H C}(\phi )\), we define a new subclass \(\mathcal {HC}_n(\phi )\) of close-to-convex harmonic mappings as follows:
Definition 1.3
A harmonic mapping \(f=h+\overline{g}\in \mathcal {H}\) is said to be in the class \(\mathcal {HC}_n(\phi )\) if \(h\in \mathcal {C}(\phi )\) and g satisfies the condition (1.5).
In 2019, Sun et al. [51] investigated upper bounds of the third Hankel determinants for the class \(\mathcal {M}(\alpha ,1,1)\) of close-to-convex harmonic mappings. In recent years, the Toeplitz determinants and Hankel determinants of functions in the class \(\mathcal {S}\) or its subclasses have attracted many researchers’ attention (see [11, 17, 19, 20, 28, 29, 33,34,35,36]). Among them, the symmetric Toeplitz determinant \(|T_q(n)|\) for subclasses of \(\mathcal {S}\) with small values of n and q, are investigated by [2, 7, 10, 49, 54, 58].
The symmetric Toeplitz determinant \(T_q(n)\) for analytic functions f is defined as follows:
where \(n,q\in {\mathbb {N}}\) and \(a_1=1\). In particular, for functions in starlike and convex classes, \(T_{2}(2)[f],\, T_{3}(1)[f]\) and \(T_{3}(2)[f]\) were studied by Ali \(et\ al.\) [7].
Let \( \mathcal {B} \) be the class of analytic functions f in \(\mathbb {D}\) such that \( |f(z)|<1 \) for all \( z\in \mathbb {D} \), and let \( \mathcal {B}_0=\{f\in \mathcal {B} : f(0)=0\} \). In 1914, Bohr [16] proved that if \( f\in \mathcal {B} \) is of the form \( f(z)=\sum _{n=0}^{\infty }a_nz^n \), then the majorant series \( M_f(r)= \sum _{n=0}^{\infty }|a_n||z|^n \) of f satisfies
for all \(z\in \mathbb {D}\) with \(|z|=r\le 1/3\), where \(f_0(z)=f(z)-f(0)\). Bohr actually obtained the inequality (1.6) for \( |z|\le 1/6 \). Moreover, Wiener, Riesz and Schur, independently, established the Bohr inequality (1.6) for \( |z|\le 1/3 \) (known as Bohr radius for the class \( \mathcal {B} \)) and proved that 1/3 is the best possible.
The Bohr phenomenon was reappeared in the 1990s due to Dixon [21]. Furthermore, Boas and Khavinson [15] found bounds for Bohr’s radius in any complete Reinhard domains. Other works one can see [3, 4, 14, 44, 45]. In recent years, Bohr inequality and Bohr radius have become an active research field in geometric function theory (see [6, 8, 27, 31, 38, 40, 43]). Furthermore, initiated by the work of [32], the Bohr’s phenomenon for the complex-valued harmonic mappings have been widely studied (see [1, 9, 25, 26, 30, 41]).
In this paper, we aim at determining the sharp estimates for Toeplitz determinants of the class \(\mathcal {M}(\alpha ,\zeta ,n)\). Moreover, we will derive an improved version of Bohr’s inequalities for the class \(\mathcal {HC}_n(\phi )\).
2 Preliminary results
To prove our main results, we need the following lemmas.
Lemma 2.1
([23, p. 41]) For a function \(p \in \mathcal {P}\) of the form (1.2), the sharp inequality \(\left| p_{n}\right| \le 2\) holds for each \(n \ge 1 .\) Equality holds for the function
Lemma 2.2
([24, Theorem 1]) Let \(p \in \mathcal {P}\) be of the form (1.2) and \(\mu \in \mathbb {C}\). Then
If \(|2 \mu -1| \ge 1\), then the inequality is sharp for the function
or its rotations. If \(|2 \mu -1|<1\), then the inequality is sharp for
or its rotations.
Lemma 2.3
([56]) Let \(f=h+\overline{g}\in \mathcal {M}(\alpha ,\zeta ,n)\). Then the coefficients \(a_k\ (k\in {\mathbb {N}}\setminus \{1\})\) of h satisfy
Moreover, the coefficients \(b_k\ (k=n+1, n+2, \ldots ; n\in {\mathbb {N}})\) of g satisfy
The bounds are sharp for the extremal function given by
Lemma 2.4
([56]) Let \(f\in \mathcal {M}(\alpha ,\zeta ,n)\) with \(0\le \alpha <1\) and \(0\le \zeta <\frac{1}{2n-1}\ (n\in {\mathbb {N}})\). Then
where
and
All these bounds are sharp, the extremal function is \(f_{\alpha ,\zeta ,n}=h_{\alpha }+\overline{g_{\alpha ,\zeta ,n}}\) or its rotations, where
The following two results are due to Ma and Minda [42].
Lemma 2.5
Let \(f \in \mathcal {C}(\phi )\). Then \(zf''(z)/f'(z) \prec zK''(z)/K'(z)\) and \(f'(z) \prec K'(z)\), where K is given by (1.4).
Lemma 2.6
Assume that \(f \in \mathcal {C}(\phi )\) and \(|z|=r<1\). Then
where K is given by (1.4). Equality holds for some \(z \ne 0\) if and only if f is a rotation of K.
Lemma 2.7
([13]) Let \(f(z)=\sum _{n=0}^{\infty } a_{n}z^{n}\) and \(g(z)=\sum _{n=0}^{\infty } b_{n}z^{n}\) be two analytic functions in \(\mathbb {D}\) and \(g \prec f\). Then
for \(|z|=r \le 1/3.\)
Remark 2.1
Lemma 2.7 continues to hold for quasi-subordination (cf. [5]). Moreover, the bound 1/3 is optimal as shown by [48, Lemma 1].
3 Toeplitz determinants for the class \(\mathcal {M}(\alpha ,\zeta ,n)\)
In this section, we will give several sharp estimates for Toeplitz determinants \(|T_{q}(n)[\cdot ]|\) of functions in the class \(\mathcal {M}(\alpha ,\zeta ,n)\).
Theorem 3.1
Let \(f\in \mathcal {M}(\alpha ,\zeta ,n)\). Then
and
The inequalities in (3.1) and (3.2) are sharp for the extremal function given by (2.3).
Proof
Suppose that \(f\in \mathcal {M}(\alpha ,\zeta ,n)\). By Lemma 2.3, we see that
yields (3.1). Equality in (3.3) holds for the function h given by
By virtue of (2.2), we get the assertion (3.2). The proof of Theorem 3.1 is thus completed. \(\square \)
Corollary 3.1
Let \(f\in \mathcal {M}(\alpha ,\zeta ,2)\). Then
and
The inequalities in (3.5) and (3.6) are sharp for the extremal function given by (2.3) with \(n=2\).
Theorem 3.2
Let \(f\in \mathcal {M}(\alpha ,\zeta ,1)\). Then
and
The inequality in (3.7) is sharp for the function h given by (3.4), and the inequality in (3.8) is sharp for the function g defined by
Proof
For \(f\in \mathcal {M}(\alpha ,\zeta ,1)\), we see that
It follows that
From (3.10), we obtain
By virtue of Lemma 2.2 and (3.11), we get
In what follows, we shall prove that the equality in (3.12) holds for the function h given by (3.4). It follows from (3.4) that
Therefore, we obtain
The graph of \(|T_{3}(1)[h]|\) with \(\alpha \in \) \([-1/2, 1)\) is presented as Fig. 1.
By the power series representations of h and g for \(f=h+\overline{g} \in \mathcal {M}(\alpha ,\zeta ,1)\), we find that
which implies that
Thus, by Lemma 2.1, (3.11) and (3.15), we deduce that the assertion (3.8) of Theorem 3.2 is true. The sharpness of (3.8) follows from (3.7). \(\square \)
Theorem 3.3
Let \(f\in \mathcal {M}(\alpha ,\zeta ,2)\). Then
and
The inequality in (3.16) is sharp for the function h given by (3.4), and the inequality in (3.17) is sharp for the function g defined by
.
Proof
Suppose that \(f\in \mathcal {M}(\alpha ,\zeta ,2)\). It follows that
In view of (3.11) and Lemma 2.1, we find that
Next, we shall maximize \(\left| a_{2}^{2}-2 a_{3}^{2}+a_{2} a_{4}\right| \). With the help of (3.11), Lemma 2.1 and Lemma 2.2, we get
Therefore, combining (3.19) with (3.20), we obtain (3.16). By noting that for \(f\in \mathcal {M}(\alpha ,\zeta ,2)\), we have
By means of Lemma 2.1, we get the assertion (3.17). The sharpness of (3.16) and (3.17) are similar to that of Theorem 3.2, we choose to omit the details here. \(\square \)
Remark 3.1
By setting \(\alpha =0\) in Corollary 3.1, Theorem 3.2 and Theorem 3.3, respectively, we get \(|T_{2}(2)[h]|\le 2\), \(|T_{3}(1)[h]|\le 4\) and \(|T_{3}(2)[h]|\le 4\). The bounds for convex functions were recently proved by Ali et al. [7, Theorem 2.11].
4 Bohr inequality for the class \(\mathcal {HC}_n(\phi )\)
In this section, we firstly give the sharp growth estimate for the class \(\mathcal {HC}_n(\phi )\).
Proposition 4.1
Let \(f \in \mathcal {HC}_n(\phi )\). Then
where
and
The bounds are sharp for the extremal function \(f_{\zeta }=h_{\zeta }+\overline{g_{\zeta }}\) with \(h_{\zeta }=K\), where K satisfies (1.4) or its rotations and \(g_{\zeta }\) satisfies \(g'_{\zeta }=\zeta z^n h'_{\zeta }\).
Proof
Let \(f=h+\overline{g} \in \mathcal {HC}_n(\phi )\). By Lemma 2.6, we know that
Let \(\gamma \) be the linear segment joining 0 to z in \(\mathbb {D}\). Then, we see that
Combining (4.4) and (4.5), we obtain
Let \(\Gamma \) be the preimage of the line segment joining 0 to f(z) under the function f. It follows that
In view of (4.6) and (4.8), we deduce that
To show the sharpness, we consider the function \(f_{\zeta }=h_{\zeta }+\overline{g_{\zeta }}\) with \(h_{\zeta }=K\) or its rotations. It is easy to see that \(h_{\zeta }=K \in \mathcal {C}(\phi )\) and \(g_{\zeta }\) satisfies \(g'_{\zeta }(z)=\zeta z^n h'_{\zeta }(z)\), which shows that \(f_{\zeta }\in \mathcal {HC}_n(\phi )\). The equality holds on both sides of (4.4) for suitable rotations of K. For \(0\le \zeta < 1/{(2n-1)}\), we see that \(f_{\zeta }(r)=R(\zeta ,n,r)\) and \(f_{\zeta }(-r)=-L(\zeta ,n,r)\). Hence \(|f_{\zeta }(r)|=R(\zeta ,n,r)\) and \(|f_{\zeta }(-r)|=L(\zeta ,n,r)\). This completes the proof of Proposition 4.1. \(\square \)
Proposition 4.2
Let \(f \in \mathcal {HC}_n(\phi )\) and \(S_{r}\) be the area of the image \(f(\mathbb {D}_{r})\) \(\mathrm{(}\mathbb {D}_{r}:=\{z\in \mathbb {C}:|z|< r\le 1\}\mathrm{)}\). Then
Proof
Let \(f=h+\overline{g} \in \mathcal {HC}_n(\phi )\). Then, the area of image of \(\mathbb {D}_{r}\) under a harmonic mapping f is given by
Since \(h\in \mathcal {C}(\phi )\), in view of (4.4) and (4.11), we have
Therefore, the assertion (4.10) of Proposition 4.2 follows directly from (4.12). \(\square \)
In what follows, we derive the Bohr inequality for the class \(\mathcal {HC}_n(\phi )\).
Theorem 4.1
Let \(f \in \mathcal {HC}_n(\phi )\). Then the majorant series of f satisfies the inequality
for \(|z|=r\le \min \{1/3,r_{f}\}\), where \(r_{f}\) is the smallest positive root in (0, 1) of
and \(L(\zeta ,n,1)\) is given by (4.2) with \(r=1\).
Proof
Let \(f=h+\overline{g} \in \mathcal {HC}_n(\phi )\). Since \(h \in \mathcal {C}(\phi )\), from Lemma 2.5, we know that
Let \(K(z)=z+\sum \limits _{n=2}^{\infty } k_{n}z^{n}\). In view of Lemma 2.7 and (4.14), we have
for \(|z|=r\le 1/3\). By integrating (4.15) with respect to r from 0 to r, we get
From the definition of \(\mathcal {HC}_n(\phi )\), we know that
This relationship along with (4.15) yields
By integrating (4.17) with respect to r from 0 to r, it follows that
Therefore, for \(|z|=r\le 1/3\), from (4.16) and (4.18), we obtain
In view of (4.1), it is evident that the Euclidean distance between f(0) and the boundary of \(f(\mathbb {D})\) is given by
We note that \(R_{\mathcal {C}}(n,r) \le L(\zeta ,n,1)\) whenever \(r \le r_{f}\), where \(r_{f}\) is the smallest positive root of \(R_{\mathcal {C}}(n,r)=L(\zeta ,n,1)\) in (0, 1). Let
Then \(H_{1}(n,r)\) is a continuous function in [0, 1]. Since
it follows that
On the other hand,
Therefore, \(H_{1}\) has a root in (0, 1). Let \(r_{f}\) be the smallest root of \(H_{1}\) in (0, 1). Then \(R_{\mathcal {C}}(n,r)\le L(\zeta ,n,1)\) for \(r\le r_{f}\). Now, in view of the inequalities (4.19) and (4.20) with the relationship \(R_{\mathcal {C}}(n,r)\le L(\zeta ,n,1)\) for \(r\le r_{f}\), we obtain
for \(|z|=r\le \min \{1/3, r_{f}\}\). \(\square \)
For a particular choice of \(\phi \) in Theorem 4.1, we get the following result.
Corollary 4.1
Let \(f \in \mathcal {M}(\alpha ,\zeta ,n)\) with \(0\le \alpha < 1\) and \(0 \le \zeta <1/(2n-1)\). Then the inequality (4.13) holds for \(|z|=r \le r_{f}\), where \(r_{f}\) is the smallest root in (0, 1) of
The radius \(r_{f}\) is sharp.
Proof
From Lemma 2.4, the Euclidean distance between f(0) and the boundary of \(f(\mathbb {D})\) shows that
We note that \(r_{f}\) is the root of the equation \(R(\alpha ,\zeta ,n,r)=L(\alpha ,\zeta ,n,1)\) in (0, 1). The existence of the root is ensured by the relation \(R(\alpha ,\zeta ,n,1) >L(\alpha ,\zeta ,n,1)\) with (2.4). For \(0<r\le r_{f}\), it is evident that \(R(\alpha ,\zeta ,n,r)\le L(\alpha ,\zeta ,n,1)\). In view of Lemma 2.3 and (4.23), for \(|z|=r\le r_{f}\), we have
To show the sharpness of the radius \(r_{f}\), we consider the function \(f=f_{\alpha ,\zeta ,n}\), which is defined in Lemma 2.4. We see that \(f_{\alpha ,\zeta ,n}\) belongs to \(\mathcal {M}(\alpha ,\zeta ,n)\). Since the left side of the growth inequality in Lemma 2.4 holds for \(f=f_{\alpha ,\zeta ,n}\) or its rotations, we have \(d(f(0), \partial f(\mathbb {D}))=L(\alpha ,\zeta ,n,1)\). Therefore, the function \(f=f_{\alpha ,\zeta ,n}\) for \(|z|=r_{f}\) gives
which reveals that the radius \(r_{f}\) is the best possible. \(\square \)
The roots \(r_{f}\) of \(F_{n}(r)=0\) for different values of \(\alpha \), \(\zeta \) and n have been shown in Tables 1, 2 and Fig. 2, respectively.
Remark 4.1
For \(n=1\) and \(\left| \zeta \right| \le 1\), \(r_{f}\) can be found in [9]. For \(\alpha =0.5\), when \(n\rightarrow \infty \), the sharp radius is 0.500000. For \(\alpha =0.9\), when \(n\rightarrow \infty \), the sharp radius is 0.815323. For \(n=1\), when \(\alpha \rightarrow 1\), the sharp radius is 0.645751.
Now, we give an improved version of Bohr inequality for the class \(\mathcal {HC}_n(\phi )\). By adding area quantity \({S_{r}}/{(2 \pi )}\) with the majorant series of \(f \in \mathcal {HC}_n(\phi )\), the sum is still less than \(d(f(0),\partial f(\mathbb {D}))\) for some radius \(r \le \min \{1/3,\widetilde{r}_{f}\}<1\).
Note that the additional term such as \({S_{r}}/{(2 \pi )}\) to the majorant sum was first mooted by Kayumov and Ponnusamy [31] to refine and improve the Bohr inequality. This variation of Bohr inequality was proved for harmonic mappings in [25]. Subsequently, several extensions were made by many authors (cf. [39]).
Theorem 4.2
Let \(f \in \mathcal {HC}_n(\phi )\) and \(S_{r}\) be the area of the image \(f(\mathbb {D}_{r})\). Then the inequality
holds for \(|z|=r\le \min \{1/3,\widetilde{r}_{f}\}\), where \(\widetilde{r}_{f}\) is the smallest positive root in (0, 1) of
and \(L(\zeta ,n,1)\) is given by (4.2) with \(r=1\).
Proof
Let \(f \in \mathcal {HC}_n(\phi )\) be of the form (1.1). Then, from the right hand inequality in (4.10) and (4.19), we obtain
for \(r\le 1/3\). Suppose that \(H_{2}(n, r)=\widetilde{R}_{f}(n,r)-L(\zeta ,n,1)\). Then \(H_{2}(n,r)\) is a continuous function in [0, 1]. The inequality (4.22) yields that \(H_{2}(n,0)=-L(\zeta ,n,1)<0\). By virtue of (4.21), we get
For \(|\zeta |\le 1/(2n-1)\), we observe that
and hence
From (4.24) and (4.25), we obtain
Since \(H_{2}(n,0)<0\) and \(H_{2}(n,1)>0\), \(H_{2}\) has a root in (0, 1) and choose \(\widetilde{r}_{f}\) to be the smallest root in (0, 1), we know that \(\widetilde{R}_{f}(n,r)\le L(\zeta ,n,1)\) for \(r \le \widetilde{r}_{f}\). Therefore, by virtue of (4.20) and (4.24), we conclude that
for \(r \le \min \{1/3, \widetilde{r}_{f}\}\). \(\square \)
Remark 4.2
By setting \(n=1\) in Theorems 4.1 and 4.2, we get the corresponding results obtained in [9].
Data availability
No data, models, or code were generated or used during the study (e.g. opinion or dateless paper).
References
Ahamed, M.B., Allu, V., Halder, H.: Bohr radius for certain classes of close-to-convex harmonic mappings. Anal. Math. Phys. 11, 1–30 (2021)
Ahuja, O.P., Khatter, K., Ravichandran, V.: Toeplitz determinants associated with Ma-Minda classes of starlike and convex functions. Iran. J. Sci. Technol. Trans. Sci. 45, 2021–2027 (2021)
Aizenberg, L.: Multidimensional analogues of Bohr’s theorem on power series. Proc. Am. Math. Soc. 128, 1147–1155 (2000)
Aizenberg, L., Aytuna, A., Djakov, P.: An abstract approach to Bohr phenomenon. Proc. Am. Math. Soc. 128, 2611–2619 (2000)
Alkhaleefah, S., Kayumov, I., Ponnusamy, S.: On the Bohr inequality with a fixed zero coefficient. Proc. Am. Math. Soc. 147, 5263–5274 (2019)
Ali, R.M., Abdulhadi, Z., Ng, Z.C.: The Bohr radius for starlike logharmonic mappings. Complex Var. Elliptic Equ. 61, 1–14 (2016)
Ali, M.F., Thomas, D.K., Vasudevarao, A.: Toeplitz determinants whose elements are the coefficients of analytic and univalent functions. Bull. Aust. Math. Soc. 97, 253–264 (2018)
Allu, V., Halder, H.: Bohr radius for certain classes of starlike and convex univalent functions. J. Math. Anal. Appl. 493, 124519 (2021)
Allu, V., Halder, H.: The Bohr inequality for certain harmonic mappings. Indag. Math. (N.S.) (2021). https://doi.org/10.1016/j.indag.2021.12.004
Arif, M., Raza, M., Tang, H., Hussain, S., Khan, H.: Hankel determinant of order three for familiar subsets of analytic functions related with sine function. Open Math. 17, 1615–1630 (2019)
Babalola, K.O.: Inequality theory and applications. In: Cho, Y.J., Kim J.K., Dragomir S.S. (eds.) On \(H_3(1)\) Hankel Determinant for Some Classes of Univalent Functions, p. 7. Nova Science Publishers Inc., New York (2011)
Bharanedhar, S.V., Ponnusamy, S.: Coefficient conditions for harmonic univalent mappings and hypergeometric mappings. Rocky Mt. J. Math. 44, 753–777 (2014)
Bhowmik, B., Das, N.: Bohr phenomenon for subordinating families of certain univalent functions. J. Math. Anal. Appl. 462, 1087–1098 (2018)
Blasco, O.: The Bohr radius of a Banach space: in vector measures, integration and related topics. Oper. Theory Adv. Appl. 201, 59–64 (2010)
Boas, H.P., Khavinson, D.: Bohr’s power series theorem in several variables. Proc. Am. Math. Soc. 125, 2975–2979 (1997)
Bohr, H.: A theorem concerning power series. Proc. Lond. Math. Soc. 2, 1–5 (1914)
Cho, N.E., Kumar, S., Kumar, V.: Hermitian-Toeplitz and Hankel determinants for certain starlike functions. Asian-Eur. J. Math. (2021). https://doi.org/10.1142/S1793557122500425
Clunie, J., Sheil-Small, T.: Harmonic univalent functions. Ann. Acad. Sci. Fenn. Ser. A. I. Math. 9, 3–25 (1984)
Cudna, K., Kwon, O.S., Lecko, A., Sim, Y.J., Śmiarowska, B.: The second and third-order Hermitian Toeplitz determinants for starlike and convex functions of order \(\alpha \). Bol. Soc. Mat. Mex. 26, 361–375 (2020)
Dobosz, A.: The third-order Hermitian Toeplitz determinant for alpha-convex functions. Symmetry 13(7), 1274 (2021)
Dixon, P.G.: Banach algebras satisfying the non-unital von Neumann inequality. Bull. Lond. Math. Soc. 27, 359–362 (1995)
Duren, P.: Harmonic Mappings in the Plane. Cambridge Univ Press, Cambridge (2004)
Duren, P.: Univalent Functions. Springer-Verlag, Berlin (1983)
Efraimidis, I.: A generalization of Livingston’s coefficient inequalities for functions with positive real part. J. Math. Anal. Appl. 435, 369–379 (2016)
Evdoridis, S., Ponnusamy, S., Rasila, A.: Improved Bohr’s inequality for locally univalent harmonic mappings. Indag. Math. (N.S.) 30, 201–213 (2019)
Huang, Y., Liu, M.-S., Ponnusamy, S.: Bohr-type inequalities for harmonic mappings with a multiple zero at the origin. Mediterr. J. Math. 18, 1–22 (2021)
Ismagilov, A., Kayumov, I.R., Ponnusamy, S.: Sharp Bohr type inequality. J. Math. Anal. Appl. 489, 124147 (2020)
Jastrzȩbski, P., Kowalczyk, B., Kwon, O.S., Lecko, A.: Hermitian Toeplitz determinants of the second and third-order for classes of close-to-star functions. RACSAM Rev. R. Acad. A. 114, 1–14 (2020)
Janteng, A., Halim, S.A., Darus, M.: Hankel determinant for starlike and convex functions. Int. J. Math. Anal. 1, 619–625 (2007)
Kayumov, I.R., Ponnusamy, S.: Bohr’s inequalities for the analytic functions with lacunary series and harmonic functions. J. Math. Anal. Appl. 465, 857–871 (2018)
Kayumov, I.R., Ponnusamy, S.: Improved version of Bohr’s inequalities. C. R. Math. Acad. Sci. Paris 358, 615–620 (2020)
Kayumov, I.R., Ponnusamy, S., Shakirov, N.: Bohr radius for locally univalent harmonic mappings. Math. Nachr. 291, 1751–1768 (2018)
Kowalczyk, B., Kwon, O.S., Lecko, A., Sim, Y.J., Śmiarowska, B.: The third-order Hermitian Toeplitz determinant for classes of functions convex in one direction. Bull. Malays. Math. Sci. Soc. 43, 3143–3158 (2020)
Kumar, V., Kumar, S.: Bounds on Hermitian-Toeplitz and Hankel determinants for strongly starlike functions. Bol. Soc. Mat. Mex. 27, 1–16 (2021)
Lecko, A., Śmiarowska, B.: Sharp bounds of the Hermitian Toeplitz determinants for some classes of close-to-convex functions. Bull. Malays. Math. Sci. Soc. 44, 3391–3412 (2021)
Lecko, A., Sim, Y.J., Śmiarowska, B.: The fourth-order Hermitian Toeplitz determinant for convex functions. Anal. Math. Phys. 10, 1–11 (2020)
Lewy, H.: On the non-vanishing of the Jacobian in certain one-to-one mappings. Bull. Am. Math. Soc. 42, 689–692 (1936)
Liu, G.: Bohr-type inequality via proper combination. J. Math. Anal. Appl. 503, 125308 (2021)
Liu, G., Liu, Z.-H., Ponnusamy, S.: Refined Bohr inequality for bounded analytic functions. Bull. Sci. Math. 173, 103054 (2021)
Liu, M.-S., Ponnusamy, S.: Multidimensional analogues of refined Bohr’s inequality. Proc. Am. Math. Soc. 149, 2133–2146 (2021)
Liu, Z.-H., Ponnusamy, S.: Bohr radius for subordination and \(k\)-quasiconformal harmonic mappings. Bull. Malays. Math. Sci. Soc. 42, 2151–2168 (2019)
Ma, W. C., Minda, D.: A unified treatment of some special classes of univalent functions, In: Proceedings of the Conference on Complex Analysis (Tianjin, 1992). Conf. Proc. Lecture Notes Anal. I, Int. Press, Cambridge, pp. 157–169 (1992)
Muhanna, Y.A., Ali, R.M., Ng, Z.C., Hasni, S.F.M.: Bohr radius for subordinating families of analytic functions and bounded harmonic mappings. J. Math. Anal. Appl. 420, 124–136 (2014)
Muhanna, Y.A.: Bohr’s phenomenon in subordination and bounded harmonic classes. Complex Var. Elliptic Equ. 55, 1071–1078 (2010)
Paulsen, V.I., Singh, D.: Bohr inequality for uniform algebras. Proc. Am. Math. Soc. 132, 3577–3579 (2004)
Ponnusamy, S., Rasila, A.: Planar harmonic and quasiregular mappings. Topics in Modern Function Theory: Chapter in CMFT, In: RMS-Lecture Notes Series, vol. , pp. 267–333 (2013)
Ponnusamy, S., Kaliraj, A.S.: Constants and characterization for certain classes of univalent harmonic mappings. Mediterr. J. Math. 12, 647–665 (2015)
Ponnusamy, S., Vijayakumar, R., Wirths, K.-J.: Improved Bohr’s phenomenon in quasi-subordination classes. J. Math. Anal. Appl. 506, 125645 (2022)
Radhika, V., Sivasubramanian, S., Murugusundaramoorthy, G., Jahangiri, J.M.: Toeplitz matrices whose elements are the coefficients of functions with bounded boundary rotation. J. Complex Anal. 2016, 4 (2016)
Sharma, P., Raina, R.K., Sokół, J.: Certain Ma-Minda type classes of analytic functions associated with the crescent-shaped region. Anal. Math. Phys. 9, 1887–1903 (2019)
Sun, Y., Wang, Z.-G., Rasila, A.: On third Hankel determinants for subclasses of analytic functions and close-to-convex harmonic mappings. Hacet. J. Math. Stat. 48, 1695–1705 (2019)
Sun, Y., Jiang, Y.-P., Rasila, A.: On a certain subclass of close-to-convex harmonic mappings. Complex Var. Elliptic Equ. 61, 1627–1643 (2016)
Thomas, D. K., Tuneski, N., Vasudevarao, A.: Univalent Functions: A primer. De Gruyter Studies in Mathematics, vol. 69. De Gruyter, Berlin, (2018)
Wang, D.-R., Huang, H.-Y., Long, B.-Y.: Coefficient problems for subclasses of close-to-star functions. Iran. J. Sci. Technol. Trans. Sci. 45, 1071–1077 (2021)
Wang, Z.-G., Huang, X.-Z., Liu, Z.-H., Kargar, R.: On quasiconformal close-to-convex harmonic mappings involving starlike functions. Acta Math. Sin. (Chin. Ser.) 63, 565–576 (2020)
Wang, Z.-G., Liu, Z.-H., Rasila, A., Sun, Y.: On a problem of Bharanedhar and Ponnusamy involving planar harmonic mappings. Rocky Mt. J. Math. 48, 1345–1358 (2018)
Wani, L.A., Swaminathan, A.: Starlike and convex functions associated with a nephroid domain. Bull. Malays. Math. Sci. Soc. 44, 79–104 (2021)
Zhang, H.-Y., Srivastava, R., Tang, H.: Third-order Hankel and Toeplitz determinants for starlike functions connected with the sine function. Mathematics 7, 404 (2019)
Acknowledgements
The present investigation was supported by the Key Project of Education Department of Hunan Province under Grant no. 19A097, and the Natural Science Foundation of Hunan Province under Grant no. 2018JJ2074 of the P. R. China. The authors would like to thank the referees for their valuable comments and suggestions, which was essential to improve the quality of this paper.
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Wang, XY., Wang, ZG., Fan, JH. et al. Some properties of certain close-to-convex harmonic mappings. Anal.Math.Phys. 12, 28 (2022). https://doi.org/10.1007/s13324-021-00642-w
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DOI: https://doi.org/10.1007/s13324-021-00642-w
Keywords
- Univalent harmonic mappings
- Close-to-convex harmonic mappings
- Bohr radius
- Toeplitz determinant
- Ma-Minda convex function