Citation: Lina Ma, Shuhai Li, Huo Tang. Geometric properties of harmonic functions associated with the symmetric conjecture points and exponential function[J]. AIMS Mathematics, 2020, 5(6): 6800-6816. doi: 10.3934/math.2020437
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Let A be the class of functions h of the form
h(z)=z+∞∑k=2akzk, | (1.1) |
where h is analytic in U={z∈C:|z|<1}.
We denote S,S∗ and K the subclasses of A consisting of univalent, starlike and convex functions respectively ([1,2]) and denote P={p:p(0)=1,Rep(z)>0,z∈U}.
An analytic function s:U={z:|z|<1}→C is subordinate to an analytic function t:U→C, if there is a function ν satisfying ν(0)=0and|ν(z)|<1(z∈U), such that s(z)=t(ν(z))(z∈U). Note that s(z)≺t(z). Especially, if t is univalent in U, then the following conclusion is true (see [1]):
s(z)≺t(z)⟺s(0)=t(0)ands(U)⊂t(U). |
In 1933, a classical Fekete-Szegö problem for h(z)=z+∞∑n=2anzn∈S was introduced by Fekete and Szegö [3] as follows,
|a3−μa22|≤{3−4μ,μ≤0,1+2exp(−2μ1−μ),0≤μ≤1,4μ−3,μ≥1. |
The result is sharp.
Using the subordination, the classes S∗(ϕ) and K(ϕ) of starlike and convex functions were defined by Ma and Minda [4] in 1994. The function h(z)∈S∗(ϕ) iff zh′(z)h(z)≺ϕ(z) and zh″(z)h′(z)≺ϕ(z), where h∈A and ϕ∈P. Moreover, Fekete-Szegö problems of the classes were obtained by Ma and Minda [4]. The problem of Fekete-Szegö has always been a hot topic in geometry function theory. Many authors studied and obtained many results (see [5,6,7]).
Let ϕ(z)=1+Az1+Bz and −1≤B<A≤1. The classes S∗(ϕ) and K(ϕ) reduce to S∗(1+Az1+Bz) and K(1+Az1+Bz), which are the classes of Janowski starlike and convex functions respectively (see [8]).
Without loss of generality, both S∗(1+z1−z)=S∗ and K(1+z1−z)=K represent the well-known classes of starlike and convex function respectively.
In 2015, Mediratta et al. [9] introduced the family of exponential starlike functions S∗(ez), that is
S∗(ez)={h∈A:zh′(z)h(z)≺ez,z∈U} |
or, equivalently
S∗(ez)={h∈A:|logzh′(z)h(z)|<1,z∈U}. |
According to the properties of the exponential function ez and the subordination relationship, the class S∗(ez) maps the unit disc U onto a region, which is symmetric with respect to the real axis and 1.
In 1959, the class S∗s of starlike functions with respect to symmetric points was introduced by Sakaguchi [10]. The function h∈S∗s if and only if
Rezh′(z)h(z)−h(−z)>0. |
In 1987, the classes S∗c and S∗cs of starlike functions with respect to conjugate points and symmetric conjugate points were introduced by El-Ashwa and Thomas [11] as follows,
h∈S∗c⟺Rezh′(z)h(z)+¯h(¯z)>0andh∈S∗sc⟺Rezh′(z)h(z)−¯h(−¯z)>0. |
For analytic functions h(z) and g(z)(z∈U). Let SH define the class of harmonic mappings with the following form (see [12,13])
f(z)=h(z)+¯g(z),z∈U, | (1.2) |
where
h(z)=z+∞∑k=2akzkandg(z)=∞∑k=1bkzk,|b1|=α∈[0,1). | (1.3) |
In particular, h is called the analytic part and g is called the co-analytic part of f.
It is well known that the function f=h+¯g is locally univalent and sense preserving in U if and only if |h′(z)|>|g′(z)|(z∈U)([14]).
According to the above conclusion, the coefficient estimations, distortion theorems, integral expressions, Jacobi estimates and growth condition in geometric properties of covering theorem of the co-analytic part can be obtained by using the analytic part of harmonic functions. In the recent years, various subclasses of SH were researched by many authors as follows.
In 2007, the subclass of SH with h∈K was studied by Klimek and Michalski [15].
In 2014, the subclass of SH with h∈S was studied by Hotta and Michalski [16].
In 2015, the subclasses of SH with h∈S∗(1+(1−2β)z1−z) and h∈K(1+(1−2β)z1−z) were studied by Zhu and Huang [17].
In this paper, by using subordination relationship, we studied the subclasses of SH with h(z)−¯h(−¯z)2∈S∗(ez) and h(z)−¯h(−¯z)2∈K(ez).
Definition 1. Suppose f=h+¯g∈SH of the form (1.3). Let HS∗,αsc(e) denote the class of harmonic univalent exponential starlike functions with symmetric conjecture point consisting of f with h∈S∗sc(e). That is, the function f=h+¯g∈HS∗,αsc(e) if and only if
2zh′(z)h(z)−¯h(−¯z)≺ez. |
Also, let HKαsc(e) denote the class of harmonic univalent convex exponential functions with symmetric conjecture point consisting of f with h∈Ksc(e), that is, f=h+¯g∈HKαsc(e) if and only if
2(zh′(z))′(h(z)−¯h(−¯z))′≺ez. |
We know that h(z)∈Ksc(e)⟺zh′(z)∈S∗sc(e).
In order to obtain our results, we need Lemmas as follows.
Lemma 1. ([18]). Let ω(z)=c0+c1z+…+cnzn+… be analytic satisfying |ω(z)|≤1 in U. Then
|cn|≤1−|c0|2,n=1,2,…, | (2.1) |
and
|c2−γc21|≤max{1,|γ|}. | (2.2) |
Lemma 2. Let
2zh′(z)h(z)−¯h(−¯z)=p(z), |
we have
h(z)=∫z0p(η)exp∫η0p(t)+¯p(−¯t)−22tdtdη. |
Lemma 3. If h(z)=z+∞∑n=2anzn∈S∗sc(e), then
|a2n|≤(2n−1)!!(2n)!!and|a2n+1|≤(2n−1)!!(2n)!!. | (2.3) |
The estimate is sharp for h given by
h(z)=1+z√1−z2−1. |
If h(z)=z+∞∑n=2anzn∈K∗sc(e), then
|a2n|≤(2n−1)!!2n(2n)!!and|a2n+1|≤(2n−1)!!(2n+1)(2n)!!. | (2.4) |
The estimate is sharp for h given by
h(z)=arcsinz−log(1+√1−z2)+log2. |
Proof. Let h(z)=z+∞∑n=2anzn∈S∗sc(e). According to Definition 1, we have
2zh′(z)h(z)−¯h(−¯z)≺ez. |
There exists a function p(z)=1+∞∑k=1pkzk satisfying
2zh′(z)h(z)−¯h(−¯z)=p(z), | (2.5) |
that is,
1+∞∑k=1pkzk≺ez=1+z+z22!+⋯. |
Using the results of Rogosinski [19], we have |pk|≤1 for k≥1.
By means of comparing the coefficients of the both sides of (2.5), we get
2na2n=p2n−1+a3p2n−3+⋯+a2n−1p1, |
and
2na2n+1=p2n+a3p2n−2+⋯+a2n−1p2. |
Let ϕ(n)=1+|a3|+⋯+|a2n−1|. It is easy to verify that
|a2n|≤12nϕ(n) | (2.6) |
and
|a2n+1|≤12nϕ(n). | (2.7) |
From (2.7), we have
ϕ(n+1)≤(2n+1)!!(2n)!!. | (2.8) |
According to (2.6), (2.7) and (2.8), we can obtain (2.3).
If h(z)=z+∞∑n=2anzn∈Ksc(e), then zh′(z)∈S∗sc(e). Using the results in (2.3), we can obtain (2.4) easily.
Lemma 4. Let μ∈C.
(1) If h(z)=z+∞∑n=2anzn∈S∗sc(e), then
|a3−μa22|≤12max{1,12|μ−1|}. | (2.9) |
(2) If h(z)=z+∞∑n=2anzn∈Ksc(e), then
|a3−μa22|≤16max{1,18|3μ−4|}. | (2.10) |
The estimates are sharp.
Proof. Let h(z)=z+∞∑n=2anzn∈S∗sc(e). According to the subordination relationship and Definition 1, we get
2zh′(z)h(z)−¯h(−¯z)=eν(z), |
that is,
log2zh′(z)h(z)−¯h(−¯z)=ν(z), | (2.11) |
where ν(z)=c1z+c2z2+⋯ is an analytic function with ν(0)=0 and |ν(z)|<1(z∈U).
By means of comparing the coefficients of two sides of (2.11), we get
a2=12c1,a3=12c2+14c21anda4=14c3+38c2c1+548c31. |
Therefore, we have
a3−μa22=12{c2−12(μ−1)c21}. |
Using the fact that (2.2) in Lemma 1, we obtain
|a3−μa22|≤12max{1,12|μ−1|}. |
The bound is sharp for h given as follows,
h(z)=∫z0exp(ξ+∫ξ0et+e−t−22tdt)dξorh(z)=∫z0exp(ξ2+∫ξ0et2−1tdt)dξ. |
Taking h(z)=z+∞∑n=2anzn∈Ksc(e)⟺zh′(z)=z+∞∑n=2nanzn∈S∗sc(e) into consideration, it is easy to obtain (2.10). The bound is sharp for h given as follows,
h(z)=∫z01η∫η0exp(ξ+∫ξ0et+e−t−22tdt)dξdηorh(z)=∫z01η∫η0exp(ξ2+∫ξ0et2−1tdt)dξdη. |
Lemma 5. Suppose h(z)∈A and |z|=r∈[0,1).
(1) Let h(z)∈S∗(e). Then
exp(−r+∫r0e−η−1ηdη)<|h′(z)|<exp(r+∫r0eη−1ηdη) | (2.12) |
and
rexp∫r0e−η−1ηdη<|h(z)|<rexp∫r0eη−1ηdη. | (2.13) |
(2) Let h(z)∈K(e). Then
exp∫r0e−η−1ηdη<|h′(z)|<exp∫r0eη−1ηdη | (2.14) |
and
rexp∫r0e−η−12ηdη<|h(z)|<rexp∫r0eη−12ηdη. | (2.15) |
Proof. Let h(z)∈S∗(e) and |z|=r∈[0,1). According to the subordination relationship and Definition 1, there exists an analytic function ν(z)=c1z+c2z2+⋯ satisfying ν(0)=0 and |ν(z)|<|z|, such that
zh′(z)h(z)=eν(z). |
Thus, it is concluded that
e−r<|zh′(z)h(z)|<er, | (2.16) |
that is,
e−r<Rezh′(z)h(z)<er. | (2.17) |
Since
Rezh′(z)h(z)=r∂∂rlog|h(z)|. | (2.18) |
By (2.17) and (2.18), we get
rexp∫r0e−η−1ηdη<|h(z)|<rexp∫r0eη−1ηdη. | (2.19) |
From (2.16) and (2.19), we have
rexp(−r+∫r0e−η−1ηdη)<|zh′(z)|<rexp(r+∫r0eη−1ηdη). |
Similar to the previous proof. We let h(z)∈K(e) and |z|=r∈[0,1), then
e−r<|1+zh″(z)h′(z)|<er. |
After simple calculation, we have
e−r−1<Rezh″(z)h′(z)<er−1. | (2.20) |
By (2.18) and (2.20), we get
exp∫r0e−η−1ηdη<|h′(z)|<exp∫r0eη−1ηdη. |
Using the conclusion in [19], for h(z)∈K(e), we have 2zh′(z)h(z)−1≺ez. According to the subordination relationship, we have
e−r<|2zh′(z)h(z)−1|<er, |
After simple calculation, we have
e−r−12<Rezh′(z)h(z)−1<er−12. | (2.21) |
By (2.18) and (2.21), we get
rexp∫r0e−η−12ηdη<|h(z)|<rexp∫r0eη−12ηdη. |
Therefore, we complete the proof of Lemma 5.
Lemma 6. ([20]). If h(z)∈S∗sc(e), then h(z)−¯h(−¯z)2∈S∗(e).
Lemma 7. If h(z)∈Ksc(e), then h(z)−¯h(−¯z)2∈K(e).
Lemma 8. Suppose h(z)∈A and |z|=r∈[0.1).
(1) Let h∈S∗sc(e). Then
ϕ1(r)<|h′(z)|<ϕ2(r), |
where
ϕ1(r)=exp(−r+∫r0e−η−1ηdη),ϕ2(r)=exp(r+∫r0eη−1ηdη). | (2.22) |
(2) Let h∈Ksc(e). Then
ψ1(r)<|h′(z)|<ψ2(r), |
where
ψ1(r)=1r∫r0exp(−t+∫t0e−η−1ηdη)dt,ψ2(r)=1r∫r0exp(t+∫t0eη−1ηdη)dt. | (2.23) |
Proof. Suppose h(z)∈S∗sc(e). It is quite similar to the proof of Lemma 5, we have
e−r|h(z)−¯h(−¯z)2|≤|zh′(z)|≤er|h(z)−¯h(−¯z)2|. | (2.24) |
According to Lemma 6 and (2.13) of Lemma 5, we have
rexp∫r0e−η−1ηdη<|h(z)−¯h(−¯z)2|<rexp∫r0eη−1ηdη. | (2.25) |
By (2.24) and (2.25), we can obtain (2.22).
If h(z)∈Ksc(e), then
e−r|(h(z)−¯h(−¯z))′2|≤|(zh′(z))′|≤er|(h(z)−¯h(−¯z))′2|. | (2.26) |
According to Lemmas 7 and (2.14) of Lemma 5, we have
exp∫r0e−η−1ηdη<|(h(z)−¯h(−¯z))′2|<exp∫r0eη−1ηdη. | (2.27) |
By (2.26) and (2.27), we get
exp(−r+∫r0e−η−1ηdη)≤|(zh′(z))′|≤exp(r+∫r0eη−1ηdη). | (2.28) |
By (2.28), integrating along a radial line ξ=teiθ, we obtained immediately,
|zh′(z)|≤∫r0exp(t+∫t0eη−1ηdη)dt |
The verification for the remainder of (2.23) is given as follows. Let H(z):=zh′(z), which is univalent. Suppose that ξ1∈Γ=H({z:|z|=r}) is the nearest point to the origin. By means of rotation, we suppose that ξ1>0 and z1=H−1(ξ1). Let γ={ξ:0≤ξ≤ξ1} and L=H−1(γ). If ς=H−1(ξ), then dξ=H′(ς)dς. Hence
ξ1=∫ξ10dξ=∫z10H′(ς)dς≥∫r0|H′(teiθ)|dt≥∫r0exp(−t+∫t0e−η−1ηdη)dt. |
Thus the proof of Lemma 8 is completed.
Next, the integral expressions for functions of the classes defined in Definition 1 are obtained.
Theorem 1. Let ω and ν be analytic in U with |ω(0)|=α,ν(0)=0,|ω(z)|<1 and |ν(z)|<1. If f=h+¯g∈HS∗,αsc(e). Then
f(z)=∫z0φ(ξ)dξ+¯∫z0ω(ξ)φ(ξ)dξ, | (3.1) |
where
φ(ξ)=eν(ξ)exp∫ξ0eν(t)+e¯ν(−¯t)−22tdt. | (3.2) |
Proof. Let f=h+¯g∈HS∗,αsc(e). Using Definition 1 and the subordination relationship, there exist analytic functions ω and ν satisfying ω(0)=b1,ν(0)=0,|ω(z)|<1 and |ν(z)|<1(z∈U), such that
2zh′(z)h(z)−¯h(−¯z)=eν(z), | (3.3) |
and
g′(z)=ω(z)h′(z). | (3.4) |
If we substitute z by −¯z in (3.4), we obtain
−2¯zh′(−¯z)h(−¯z)−¯h(z)=eν(−¯z). | (3.5) |
It follows from (3.4) and (3.5) that
2z(h(z)−¯h(−¯z))′h(z)−¯h(−¯z)=eν(z)+e¯ν(−¯z). | (3.6) |
A routine computation for the equality (3.6) gives rise to the following equation,
¯h(z)−h(−¯z)2=zexp∫z0eν(t)+e¯ν(−¯t)−22tdt. | (3.7) |
Plugging (3.7) back into (3.3), we have
h′(z)=eν(z)exp∫z0eν(t)+e¯ν(−¯t)−22tdt. | (3.8) |
If the equality (3.8) is integrated from the both sides of it, then
h(z)=∫z0eν(ξ)exp∫ξ0eν(t)+e¯ν(−¯t)−22tdtdξ. |
Inserting (3.8) into (3.4), it is easy to show that
g(z)=∫z0ω(ξ)eν(ξ)exp∫ξ0eν(t)+e¯ν(−¯t)−22tdtdξ. |
Thus, the proof of Theorem 1 is completed.
Taking Theorem 1 and h∈Ksc(e)⟺zh′(z)∈S∗sc(e) into consideration, we get the following result.
Theorem 2. Let ω and ν be analytic in U satisfying |ω(0)|=α,ν(0)=0,|ω(z)|<1 and |ν(z)|<1. If f∈HKαsc(e), then
f(z)=∫z01η∫η0φ(ξ)dξdη+¯∫z0ω(η)η∫η0φ(ξ)dξdη. |
where φ(ξ) is defined by (3.2).
In the following, the coefficient estimates of the class HS∗,αsc(e) will be obtained.
Theorem 3. Let h and g be given by (1.3). If f=h+¯g∈HS∗,αsc(e), then
|b2n|≤{1−α22+α2,n=1,(1−α2)2n(1+n∑k=2(4k−3)(2k−3)!!(2k−2)!!)+α(2n−1)!!(2n)!!,n≥2, | (3.9) |
and
|b2n+1|≤{2(1−α2)3+α2,n=1,(1−α2)2n+1(1+n∑k=2(4k−3)(2k−3)!!(2k−2)!!+(2n−1)!!(2n−2)!!)+α(2n−1)!!(2n)!!,n≥2. | (3.10) |
The estimates are sharp and the extremal function is
fα0(z)=1+z√1−z2−1+¯∫z0(α+(1−α2−α)t)(1−t)2√(1−t2)dt. |
Specially, if f∈HS∗,0sc(e), then
|b2n|≤{12,n=1,12n(1+n∑k=2(4k−3)(2k−3)!!(2k−2)!!),n≥2, |
and
|b2n+1|≤{23,n=1,12n+1(1+n∑k=2(4k−3)(2k−3)!!(2k−2)!!+(2n−1)!!(2n−2)!!),n≥2. |
The estimates are sharp and the extremal function is
f01(z)=1+z√1−z2−1+¯2z3+3z2−13(1−z2)32+13. |
Proof. Let h and g be given by (1.3). Using the fact that g′=ωh′ satisfying ω(z)=c0+c1z+c2z2+⋯ analytic in U, we obtain
2nb2n=2n∑p=1papc2n−p(a1=1,n≥1) | (3.11) |
and
(2n+1)b2n+1=2n+1∑p=1papc2n+1−p(a1=1,n≥1). | (3.12) |
It is easy to show that
2n|b2n|≤2n∑p=1p|ap||c2n−p| |
and
(2n+1)|b2n+1|≤2n+1∑p=1p|ap||c2n+1−p|. |
Since g′=ωh′, it follows that c0=b1. By (2.1), it is obvious that |ck|≤1−α2 for k∈N. Therefore,
|b2n|≤{1−α22+|a2|α,n=1,(1−α2)2n(1+2n−1∑k=2k|ak|)+α|a2n|,n≥2, | (3.13) |
and
|b2n+1|≤{1−α23(1+2|a2|)+|a3|α,n=1,(1−α2)2n+1(1+2n∑k=2k|ak|)+α|a2n+1|,n≥2. | (3.14) |
According to Lemma 3, (3.13) and (3.14), after the simple calculation, (3.9) and (3.10) can be obtained easily. We also obtain the extreme function.
By using the same methods in Theorem 3, the following results are obtained.
Theorem 4. Let h and g of the form (1.3). If f=h+¯g∈HKαsc(e), then
|b2n|≤{1−α24+α4,n=1,(1−α2)(2n)2(1+n∑k=2(4k−3)(2k−3)!!(2k−2)!!)+α(2n−1)!!2n(2n)!!,n≥2, |
and
|b2n+1|≤{2(1−α2)9+α6,n=1,(1−α2)(2n+1)2(1+n∑k=2(4k−3)(2k−3)!!(2k−2)!!+(2n−1)!!(2n−2)!!)+α(2n−1)!!(2n+1)(2n)!!,n≥2. |
For functions of the classes defined in the paper, Fekete-Szegö inequality of which are listed below.
Theorem 5. Let f=h+¯g with h and g given by (1.3) and μ∈C.
(1) If f∈HS∗,αsc(e), then
|b3−μb22|≤(1−α2)3{1+3|μ|(1−α2)4+|2−3μb1|2}+α2max{1,|μb1−1|2}, |
|b2n−b2n−1|≤{12(1−α2)+3α2,n=1,(1−α2)((12n+12n−1)(1+n∑k=2(4k−3)(2k−3)!!(2k−2)!!)−(2n−3)!!(2n−1)(2n−4)!!)+α((2n−1)!!(2n)!!+(2n−3)!!(2n−2)!!),n≥2, |
and
|b2n+1−b2n|≤(1−α2)((12n+1+12n)(1+n∑k=2(4k−3)(2k−3)!!(2k−2)!!)+(2n−1)!!(2n+1)(2n−2)!!)+2α(2n−1)!!(2n)!!,n≥1. |
(2) If f∈HKαsc(e), then
|b3−μb22|≤(1−α2)3{1+3|μ|(1−α2)4+|2−3μb1|4}+α6max{1,|4−3μb1|8}, |
|b2n−b2n−1|≤{12(1−α2)+5α4,n=1,(1−α2)((12n+12n−1)(1+2n∑k=2(2k−3)!!(2k−2)!!)−(2n−3)!!(2n−1)(2n−2)!!)+α((2n−1)!!(2n)(2n)!!+(2n−3)!!(2n−1)(2n−2)!!),n≥2, |
and
|b2n+1−b2n|≤(1−α2)((12n+1+12n)(1+2n∑k=2(2k−3)!!(2k−2)!!)+(2n−1)!!(2n+1)(2n)!!)+α(12n+1+12n)(2n−1)!!(2n)!!,n≥1. |
Proof. From the relation (3.11) and (3.12), we have
2b2=c1+2a2c0,3b3=c2+2a2c1+3a3c0, |
and
2nb2n=2n∑p=1papc2n−p,(2n+1)b2n+1=2n+1∑p=1papc2n+1−p(a1=1,n≥1). |
By (2.1), we have
|b3−μb22|≤1−α23{1+3|μ|(1−α2)4+|a2||2−3μb1|}+α|a3−μb1a22|, |
|b2n−b2n−1|≤{12(1−α2)+α(1+|a2|),n=1,(1−α2)(12n2n−1∑p=1p|ap|+12n−12n−2∑p=1p|ap|)+α(|a2n|+|a2n−1|),n≥2, |
and
|b2n+1−b2n|≤(1−α2)(12n+12n∑p=1p|ap|+12n2n−1∑p=1p|ap|)+α(|a2n+1|+|a2n|),n≥1. |
According to Lemma 3 and Lemma 4, we can compete the proof of Theorem 5. The estimates above are sharp.
Paralleling the results of Zhu et al.[17], the corresponding results for functions of the classes defined in the paper can be obtained. For example, the estimates of distortion, growth of g and Jacobian of f and so on.
Theorem 6. Let |z|=r∈[0,1).
(1) If f=h+¯g∈HS∗,αsc(e), then
max{α−r,0}(1−αr)ϕ1(r)≤|g′(z)|≤α+r(1+αr)ϕ2(r), | (3.15) |
where ϕ1(r) and ϕ2(r) are given by (2.22).
Especially, let α=0, we have
|g′(z)|≤rexp(r+∫r0eη−1ηdη). |
(2) If f=h+¯g∈HKαsc(e), then
max{α−r,0}(1−αr)ψ1(r)≤|g′(z)|≤(α+r)(1+αr)ψ2(r), | (3.16) |
where ψ1(r) and ψ2(r) are given by (2.23).
Especially, let α=0, we have
|g′(z)|≤∫r0exp(t+∫t0eη−1ηdη)dt. |
Proof. According to the relation g′=ωh′, it is easy to see ω(z) satisfying |ω(0)|=|g′(0)|=|b1|=α such that ([21]):
|ω(z)−ω(0)1−¯ω(0)ω(z)|≤|z|. |
It is easy to show
|ω(z)−ω(0)(1−r2)1−|ω(0)|2r2|≤r(1−|ω(0)|2)1−|ω(0)|2r2. |
A tedious calculation gives
max{α−r,0}1−αr≤|ω(z)|≤α+r1+αr,z∈U. | (3.17) |
Applying (3.17) and (2.22), we get (3.15). Similarly, applying (3.17) and (2.23), we get (3.16). Thus we complete the proof of Theorem 6.
Using the method analogous to that in proof of Lemma 8, we can obtain the following results.
Theorem 7. Let |z|=r∈[0,1).
(1) If f=h+¯g∈HS∗,αsc(e), then
∫r0max{α−ξ,0}(1−αξ)ϕ1(ξ)dξ≤|g(z)|≤∫r0α+ξ(1+αξ)ϕ2(ξ)dξ, |
where ϕ1(ξ) and ϕ2(ξ) are given by (2.22).
Especially, let α=0, we have
|g(z)|≤∫r0ξexp(ξ+∫ξ0eη−1ηdη)dξ. |
(2) If f=h+¯g∈HKαsc(e), then
∫r0max{α−ξ,0}(1−αξ)ψ1(ξ)dξ≤|g(z)|≤∫r0(α+ξ)(1+αξ)ψ2(ξ)dξ, |
where ψ1(ξ) and ψ2(ξ) are given by (2.23).
Especially, let α=0, we have
|g(z)|≤∫r0∫ξ0exp(t+∫t0eη−1ηdη)dtdξ. |
Next, the Jacobian estimates and growth estimates of f are obtained.
Theorem 8. Let |z|=r∈[0,1).
(1) If f=h+¯g∈HS∗,αsc(e), then
(1−α2)(1−r2)(1+αr)2ϕ21(r)≤Jf(z)≤{(1−α2)(1−r2)(1−αr)2ϕ22(r),r<α,ϕ22(r),r≥α., |
where ϕ1(r) and ϕ2(r) are given by (2.22).
(2) If f=h+¯g∈HKαsc(e), then
(1−α2)(1−r2)(1+αr)2ψ21(r)≤Jf(z)≤{(1−α2)(1−r2)(1−αr)2ψ22(r),r<α,ψ22(r),r≥α, |
where ψ1(r) and ψ2(r) are given by (2.23).
Proof. It is well known that Jacobian of f=h+¯g is
Jf(z)=|h′(z)|2−|g′(z)|2=|h′(z)|2(1−|ω(z)|2), | (3.18) |
where ω satisfying g′=ωh′ with ω(0)=0 and |ω(z)|<1 for z∈U.
Let f∈HS∗,αsc(e), plugging (3.17) and (2.22) back into (3.18), we get
Jf(z)≥(1−α2)(1−r2)(1+αr)2exp(−2r+2∫r0e−η−1ηdη), |
and
Jf(z)≤exp(2r+2∫r0eη−1ηdη)(1−(max{(α−r),0})2(1−αr)2)={exp(2r+2∫r0eη−1ηdη)⋅(1−α2)(1−r2)(1−αr)2,r<α,exp(2r+2∫r0eη−1ηdη),r≥α. |
Thus this completes the proof of (1). Plugging (3.17) and (2.23) back into (3.18), (2) of Theorem 8 can be proved by the same method as employed before.
Theorem 9. Let |z|=r,0≤r<1.
(1) If f=h+¯g∈HS∗,αsc(e), then
∫r0(1−α)(1−ξ)(1+αξ)ϕ1(ξ)dξ≤|f(z)|≤∫r0(1+α)(1+ξ)(1+αξ)ϕ2(ξ)dξ, | (3.19) |
where ϕ1(ξ) and ϕ2(ξ) are given by (2.22).
(2) If f=h+¯g∈HKαsc(e), then
∫r0(1−α)(1−ξ)(1+αξ)ψ1(ξ)dξ≤|f(z)|≤∫r0(1+α)(1+ξ)(1+αξ)ψ2(ξ)dξ, | (3.20) |
where ψ1(ξ) and ψ2(ξ) are given by (2.23).
Proof. For any point z=reiθ∈U, let Ur={z∈U:|z|<r} and denote
d=minz∈Ur|f(Ur)|. |
It is easy to see that U(0,d)⊆f(Ur)⊆f(U). Thus, there is zr∈∂Ur satisfying d=|f(zr)|. Let L(t)=tf(zr) for t∈[0,1], then ℓ(t)=f−1(L(t)) is a well-defined Jordan arc. For f=h+¯g∈HS∗,αsc(β), by (2.22) and (3.17), we get
d=|f(zr)|=∫L|dω|=∫ℓ|df|=∫ℓ|h′(ρ)dρ+¯g′(ρ)dˉρ|≥∫ℓ|h′(ρ)|(1−|ω(ρ)|)|dρ|≥∫ℓ(1−α)(1−|ρ|)(1+α|ρ|)exp(−|ρ|+∫|ρ|0e−η−1ηdη)|dρ|,=∫10(1−α)(1−|ℓ(t)|)(1+α|ℓ(t)|)exp(−|ℓ(t)|+∫|ℓ(t)|0e−η−1ηdη)dt,≥∫r0(1−α)(1−ξ)(1+αξ)exp(−ξ+∫ξ0e−η−1ηdη)dξ. |
Using (2.22) and (3.17), the right side of (3.19) is obtained. The remainder of proofs is similar to that in (3.20) and so we omit.
According to (3.19) and (3.20), it follows that the covering theorems of f.
Theorem 10. Let f=h+¯g∈SH.
(1) If f∈HS∗,αsc(e), then UR1⊂f(U), where
R1=∫10(1−α)(1−ξ)(1+αξ)exp(−ξ+∫ξ0e−η−1ηdη)dξ. |
(2) If f∈HKαsc(e), then UR2⊂f(U), where
R2=∫10(1−α)(1−ξ)ξ(1+αξ)∫ξ0exp(−t+∫t0e−η−1ηdη)dtdξ. |
In this paper, with the help of the analytic part h satisfying certain conditions, we obtain the coefficients estimates of the co-analytic part g and the geometric properties of harmonic functions. Applying the methods in the paper, the geometric properties of the co-analytic part and harmonic function with the analytic part satisfying other conditions can be obtained, which can enrich the research field of univalent harmonic mapping.
This work was supported by Research Program of Science and Technology at Universities of Inner Mongolia Autonomous Region(Grant No. NJZY20198; Grant No. NJZZ19209), Natural Science Foundation of Inner Mongolia Autonomous Region of China (Grant No. 2020MS01011; Grant No. 2019MS01023; Grant No. 2018MS01026) and the Program for Young Talents of Science and Technology in Universities of Inner Mongolia Autonomous Region Under Grant (Grant No. NJYT-18-A14).
The authors agree with the contents of the manuscript, and there is no conflict of interest among the authors.
[1] | P. L. Duren, Univalent Functions (Grundlehren der Mathematischen Wissenschaften 259), Springer-Verlag, New York, 1983. |
[2] | H. M. Srivastava, S. Owa, Current Topics in Analytic Function Theory, World Scientific, London, 1992. |
[3] | M. Fekete, G. Szegö, Eine bemerkung uber ungerade schlichte funktionen, J. Lond. Math. Soc., s1-8 (1933), 85-89. |
[4] | W. Ma, D. Minda, A unified treatment of some special classes of univalent functions, In: Proceeding of the Conference on Complex Analysis, International Press, Boston, USA, 1994, 157-169. |
[5] |
R. M. EL-Ashwah, A. H. Hassan, Fekete-Szegö inequalities for certain subclass of analytic functions defined by using Sălăgean operator, Miskolc Math. Notes, 17 (2017), 827-836. doi: 10.18514/MMN.2017.1495
![]() |
[6] | W. Koepf, On the Fekete-Szegö problem for close-to-convex functions, P. Am. Math. Soc., 101 (1987), 89-95. |
[7] | F. M. Sakar, S. Aytaş, H. Ö. Güney, On The Fekete-Szegö problem for generalized class Mα,γ(β) defined by differential operator, J. Nat. Appl. Sci., Süleyman Demirel University, 20 (2016), 456-459. |
[8] |
W. Janowski, Some extremal problems for certain families of analytic functions, Ann. Pol. Math., 28 (1973), 297-326. doi: 10.4064/ap-28-3-297-326
![]() |
[9] |
R. Mendiratta, S. Nagpal, V. Ravichandran, On a subclass of strongly starlike functions associated with exponential function, B. Malays. Math. Sci. Soc., 38 (2015), 365-386. doi: 10.1007/s40840-014-0026-8
![]() |
[10] |
K. Sakaguchi, On a certain univalent mapping, J. Math. Soc. JPN, 11 (1959), 72-75. doi: 10.2969/jmsj/01110072
![]() |
[11] | R. El-Ashwah, D. Thomas, Some subclasses of closed-to-convex functions, J. Ramanujan Math. Soc., 2 (1987), 85-100. |
[12] |
J. Clunie, T. Sheil-Small, Harmonic univalent functions, Ann. Acad. Sci. Fenn. Math., 9 (1984), 3-25. doi: 10.5186/aasfm.1984.0905
![]() |
[13] | P. L. Duren, Harmonic mappings in the plane, Cambridge University Press, England, 2004. |
[14] |
H. Lewy, On the non-vanishing of the Jacobian in certain one-to-one mappings, B. Am. Math. Soc., 42 (1936), 689-692. doi: 10.1090/S0002-9904-1936-06397-4
![]() |
[15] | D. Klimek, A. Michalski, Univalent anti-analytic perturbations of convex analytic mappings in the unit disc, Ann. Univ. Mariae Curie-Skłodowska Sect. A, 61 (2007), 39-49. |
[16] | I. Hotta, A. Michalski, Locally one-to-one harmonic functions with starlike analytic part, arXiv: 1404.1826, 2014. |
[17] | M. Zhu, X. Huang, The distortion theorems for harmonic mappings with analytic parts convex or starlike functions of order β, J. Math., 2015 (2015), 460191. |
[18] | G. Kohr, I. Graham, Geometric Function Theory in One and Higher Dimensions, Marcel Dekker, New York, 2003. |
[19] | W. Rogosinski, On the coefficients of subordinate functions, P. Lond. Math. Soc., 2 (1945), 48-82. |
[20] | Y. Polatoğlu, M. Bolcal, A. Sen, Two-point distortion theorems for certain families of analytic functions in the unit disc, Int. J. Math. Math. Sci., 66 (2003) 4183-4193. |
[21] | G. M. Goluzin, Geometric Theory of Functions of a Complex Variable, American Mathematical Society, Rhode Island, 1969. |
1. | 丽娜 马, A Class of Univalent Harmonic Functions with Symmetric Conjugate Points Defined by the S?l?gean-q Differential Operator, 2024, 14, 2160-7583, 103, 10.12677/pm.2024.147277 |