Sections of univalent harmonic mappings
Saminathan Ponnusamy, Anbareeswaran Sairam Kaliraj, and Victor V., Starkov

TL;DR
This paper determines the univalence radius of sections of normalized univalent harmonic mappings with convex, starlike, or close-to-convex ranges, providing sharp results especially for convex ranges, and compares with classical conformal mapping results.
Contribution
It establishes the sharp radius of univalence for sections of harmonic mappings with various geometric range conditions, extending classical conformal mapping results.
Findings
The radius of univalence for sections with convex range is sharp.
Each section $s_{n,n}(f)$ is univalent in the disk of radius 1/4 for all $n extgreater{}2$.
Results extend classical univalence radius results to harmonic mappings.
Abstract
In this article, we determine the radius of univalence of sections of normalized univalent harmonic mappings for which the range is convex (resp. starlike, close-to-convex, convex in one direction). Our result on the radius of univalence of section is sharp especially when the corresponding mappings have convex range. In this case, each section is univalent in the disk of radius for all , which may be compared with classical result of Szeg\"{o} on conformal mappings.
| Value of | Value of |
|---|---|
| 2 | 0.108193 |
| 3 | 0.147197 |
| 4 | 0.182263 |
| 5 | 0.214025 |
| 10 | 0.337088 |
| 50 | 0.675001 |
| 100 | 0.788521 |
| 287 | 0.900122 |
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Sections of univalent harmonic mappings
Saminathan Ponnusamy
S. Ponnusamy, and A. Sairam Kaliraj, Indian Statistical Institute (ISI), Chennai Centre, SETS, MGR Knowledge City, CIT Campus, Taramani, Chennai 600 113, India.
[email protected], [email protected]
,
Anbareeswaran Sairam Kaliraj
and
Victor V. Starkov
V.V. Starkov, Petrozavodsk State University, 33, Lenin Str., 185910, Petrozavodsk, Republic of Karelia, Russia.
Abstract.
In this article, we determine the radius of univalence of sections of normalized univalent harmonic mappings for which the range is convex (resp. starlike, close-to-convex, convex in one direction). Our result on the radius of univalence of section is sharp especially when the corresponding mappings have convex range. In this case, each section is univalent in the disk of radius for all , which may be compared with classical result of Szegö on conformal mappings.
Key words and phrases:
Harmonic univalent, starlike, close-to-convex and convex mappings, convex in one direction, partial sums
2010 Mathematics Subject Classification:
Primary: 30C45; Secondary: 31A05, 30C55, 32E30
File: 1701.06041.tex, printed: 2024-3-19, 17.31
1. Introduction and main results
Since confirmation of the Bieberbach conjecture by Louis de Branges [3] on the class , of all normalized univalent analytic functions defined in the unit disk , one of the open problems about the class is that of determining the precise value of such that all sections of are univalent in . Here we say that is normalized if . Also, let
[TABLE]
whenever
[TABLE]
In [24], Szegö proved that the section/partial sum of is univalent in for all . The constant is sharp as the second section of the Koebe function suggests. In [20], Robertson proved that the section is starlike in the disk for , and that the number cannot be replaced by a smaller constant. Later in the year 1991, Bshouty and Hengartner [4] showed that the Koebe function is not extremal for the problem of determining the radius of univalency of the partial sums of functions in . At this time the best known result is due to Jenkins [11] who proved that is univalent in for , where the radius of univalence is at least for . For related investigations on this topic, see the recent articles [14, 16] and the references therein. More interestingly, as investigated recently in [12, 13], our main aim in this article is to consider the analogous problem for univalent harmonic mappings in the unit disk, since harmonic mappings have interesting links with geometric function theory, minimal surfaces and locally quasiconformal mappings.
Every harmonic mapping in a simply connected domain can be written as , where and are analytic. In particular, we consider the class of all complex-valued harmonic functions in normalized by . We call and , the analytic and the co-analytic parts of , respectively, and obviously they have the following power series representation
[TABLE]
Throughout the discussion we shall use this representation. Since the Jacobian of is we say that is sense-preserving in if in . Let denote the class of all sense-preserving harmonic univalent mappings and set . For many basic results on univalent harmonic mappings, we refer to the monograph of Duren [7] and also [15]. Harmonic mappings techniques have been used to study and solve fluid flow problems (see [1]). In particular, the study of univalent harmonic functions having special geometric property such as convexity, starlikeness, and close-to-convexity arises naturally while dealing with planar fluid dynamics problems. For example, in [1, Theorem 4.5], Aleman et al. considered a fluid flow problem on a convex domain satisfying an interesting geometric property. In view of results from [17, 19], one obtains that harmonic mappings, such that on the convex domain , considered by the authors in [1, Theorem 4.5] are indeed close-to-convex in .
Another reasons in studying the sections of harmonic mappings is that approximation of real valued harmonic functions by harmonic polynomials attracted the attention of mathematicians (see [25]) as it has many advantages. For example, a harmonic function has its maximum and minimum values on the boundary of the regions of consideration. Because planar harmonic mappings defined on have series representation as in (3), sections of can be thought of as an approximation of by complex-valued harmonic polynomials and thus, approximation of univalent harmonic mappings by univalent harmonic polynomials might lead to new applications in fluid flow problems, in particular. Until recently, much is not known about the univalence of sections of univalent harmonic mappings. In 2013, Li and Ponnusamy [12, 13] initiated the study on this topic by considering certain classes of univalent harmonic mappings. However, the harmonic analog of these results are not known in the literature even for well-known geometric subclasses of , namely, the classes are , , and mapping onto, respectively, convex, starlike, and close-to-convex domains, just as , , and are the subclasses of mapping onto these respective domains. At this place, it is worth to recall that general theorems on convolutions [22] (see also [6, p. 256, 273]) allow one to conclude that is convex, starlike, or close-to-convex in the disk , for , whenever is convex (resp. starlike or close-to-convex) in .
Another interesting geometric subclass of which attracted function theorists is the class of univalent harmonic functions for which is convex in a direction . Recall that a domain is called convex in the direction if the intersection of with each line parallel to the line through [math] and is connected (or empty). See, for example, [5, 9, 21]. Now, we recall the class introduced in [18], where
[TABLE]
and as in [18], let One of the conjectures stated in [18] reads as follows.
Conjecture 1**.**
. That is, for every function , there exists at least one such that .
In [18], it was also remarked that the truth of this conjecture verifies the coefficient conjecture of Clunie and Sheil-Small for , namely,
[TABLE]
for each , where . Conjecture 1 remains open. The bound is well-known and sharp which follows from the classical Schwarz lemma. However, the conjectured bounds of Clunie and Sheil-Small have been verified for a number of subclasses of , namely, for , , and the class of harmonic mappings convex in one direction. More recently, Starkov [23] established a criteria for functions belonging to the class and as a consequence, several examples including harmonic univalent polynomials are also obtained for a given .
For with power series representation as in (3), the sections/partial sums of are defined as
[TABLE]
where and . However, the special case seems interesting in its own merit. We now state our main results.
Theorem 1**.**
Let with series representation as in (3). Suppose that belongs to any one of the following geometric subclasses of : , , or the class of harmonic mappings convex in one direction. Then the section is univalent in the disk . Here is the unique positive root of the equation , where
[TABLE]
with
[TABLE]
In particular, every section is univalent in the disk , where
[TABLE]
Moreover, , where .
For functions in the convex family of harmonic mappings, we have the following interesting result which may compared with the original conjecture for functions in .
Theorem 2**.**
Let with series representation as in (3). Then the section is univalent in the disk , where is the unique positive root of the equation . Here
[TABLE]
In particular, for , and , the harmonic function
[TABLE]
is univalent and close-to-convex in the disk . Moreover, we have , where .
It is worth to remark that if , then we actually prove that for , is stable harmonic close-to-convex (see [10]) in .
The paper is organized as follows. In Section 2, we recall certain known results which are crucial in the proof of our main theorems. In Section 3, we present the proofs of Theorems 1 and 2, and as a consequence, we state a couple of corollaries.
2. Useful Lemmas
Now, we recall some results that are needed for the proofs of our main results. The following result due to Bazilevich [2] gives the necessary and sufficient condition for a normalized analytic function to be univalent in .
Theorem A. * An analytic function defined in and determined by (2) is univalent in if and only if for each and each ,*
[TABLE]
*where , and . *
Recently, Starkov [23] generalized this result to the class of normalized sense-preserving harmonic mappings in the following form.
Theorem B. * A sense-preserving harmonic function defined in determined by (3) is univalent in if and only if for each and each ,*
[TABLE]
*where and . *
The following two point distortion theorem of Graf et al. [8] plays a crucial role in the proof of our main results.
Lemma C. * If , , , then*
[TABLE]
*where . *
Finally, we recall the following well-known identities which are also easy to derive.
Lemma 1**.**
The following identities are true for :
- (i)
.
- (ii)
.
- (iii)
.
Proof. The identity (i) is obvious. To obtain (ii) we may multiply (i) by and then differentiate it with respect to . The proof of case (iii) is similar. So, we omit its proof. ∎
3. Partial sums of Univalent Harmonic Mappings
3.1. Proof of Theorem 1
Suppose that belongs to either or or or to the class of harmonic mappings convex in one direction, where are given by the power series (3) with . Set for . Then and
[TABLE]
Evidently, finding the largest radius of univalence of is equivalent to finding the largest value such that is univalent in . From Theorem , it is clear that is univalent in if and only if is sense-preserving in and the associated section has the property that
[TABLE]
where , , , for all ,
[TABLE]
and
[TABLE]
Setting , in (8) and from the univalency of for , we get that
[TABLE]
In order to find a lower bound for , we need to find an upper bound for
[TABLE]
By the assumption on , it follows that (see for instance [7, 18])
[TABLE]
and hence
[TABLE]
From (9) and (10), we get that
[TABLE]
The inequality holds for all , whenever , where is defined by (4). This gives that for all , where is the positive root of the equation which lies in the interval . In order to complete the proof, we have to show that is locally univalent in . However, is locally univalent in if and only if the analytic functions is locally univalent in for every . That is, we have to show that for all and . It is easy to see that
[TABLE]
From the hypothesis, it is clear that belongs to either or (see for instance, [18]). As the affine spanning of as well as are linear invariant families [18],
[TABLE]
Therefore, from a well known result on linear invariant family of harmonic mappings, it follows that (see [7, p. 99])
[TABLE]
Moreover, for (see (9)), we see that
[TABLE]
and thus,
[TABLE]
where the last inequality here gives the condition . This observation proves that is univalent in the disk and the proof of the first part of the theorem is complete.
From the above discussion, it is apparent that , where . Next, we need to consider the special case and determine the lower bound for with certain restriction on . In this case, the sufficient condition (4) for the univalence of reduces to
[TABLE]
where determined from (5) may be rearranged in a convenient form as
[TABLE]
As , it is clear that the radius of univalence . Setting , where , we see that (4) holds, whenever , where
[TABLE]
From the definition of , it is clear that and hence can be chosen to be for some positive real number . However, computations shows that
[TABLE]
Therefore, we may set
It is easy to see that for all . For , we shall prove that . For , it is sufficient to prove that is a decreasing function in , whenever
[TABLE]
In order to do this, we first differentiate with respect to and obtain that , where
[TABLE]
and
[TABLE]
From the definition of , it is clear that for all , where . To conclude , we need to prove that for all and . From the grouping of terms in , one can see that for , and . Next, we show that for all . To do this, for any fixed , we set , where . Then, reduces to
[TABLE]
where
[TABLE]
A computation shows that has no real root. Moreover, the only real roots of , , and are , , and , respectively. Therefore, for , will have same sign for all . As for , we conclude that for all . This shows that for all and hence, for all . Since
[TABLE]
from the fact that , we infer that is a positive and decreasing function of in the interval , for each . To complete the proof, we have to show that for all . By making use of upper bounds of for various values of , it is easy to see that for . A direct computation using mathematica shows that for also. The proof is complete.
Corollary 1**.**
Let satisfies the hypothesis of Theorem 1. Then is univalent in the disk
- (i)
, whenever ,
- (ii)
, whenever ,
- (ii)
, whenever .
The bound for the radius of univalence of for certain values of are listed in Table 1.
The following shearing theorem due to Clunie and Sheil-Small is needed for the proof of Theorem 2.
Theorem D. [5, Theorem 5.3]* A locally univalent harmonic function in is a univalent mapping of onto a domain convex in the direction if and only if is a conformal univalent mapping of onto a domain convex in the direction . *
The proof of Theorem 2 is similar to the proof in Theorem 1 with the help of the corresponding coefficients inequalities and the sharp lower bound for the two point distortion theorem (Lemma 2) for .
Lemma 2**.**
If , , , then
[TABLE]
Proof. For every pair of points and in , we can find a such that
[TABLE]
Since , is convex in every direction and hence, by Lemma , the function is univalent in for every . The desired conclusion follows from the two point distortion theorem for univalent analytic functions (see [6, Corollary 7, p. 127]). ∎
3.2. Proof of Theorem 2
Let . Then the Taylor coefficients of and satisfy the inequality (see [5, 7])
[TABLE]
Following the proof of Theorem 1 with the same notation and (12), we get that
[TABLE]
From Lemma 2, we obtain that
[TABLE]
The inequality holds for all , whenever , where is defined by (6). However, for all , where is the unique positive root of the equation (6) which is less than . Since the affine span of is a linear invariant family and , we have (see [7, p. 99])
[TABLE]
Following the proof technique of Theorem 1, we conclude that is locally univalent in . Now, let us first consider the special case . In this case, (6) reduces to
[TABLE]
From Lemma 1, the expression for simplifies to
[TABLE]
For , if and only if , where
[TABLE]
From the continuity of and from the fact that and , it is evident that there exists a real number such that for all and . To complete the proof, we need to find the lower bound for for large values of . By letting in and making use of the fact that , for , we see that holds whenever , where
[TABLE]
Clearly and and hence the dominating term in could be at most . This allows us to choose for appropriate choices of . As for , cannot be chosen to be greater than in our estimate. Moreover, for , a computation shows that . Therefore, we may set
[TABLE]
Throughout the further discussion in this proof, we assume that since holds only when .
For , we shall prove that . We observe that it suffices to show that for , and . Indeed, differentiating (14) with respect to one can obtain by a standard calculation that
[TABLE]
whenever . As for all , we deduce that
[TABLE]
Next, we show that for all . To do this, we may rewrite the expression for , where
[TABLE]
First, we show that for all . We introduce
[TABLE]
We see that is an increasing function of in the interval and thus, we easily have
[TABLE]
Similarly, it is easy to see that is increasing in the interval and is increasing in the interval . Therefore, a simple computation shows that
[TABLE]
and
[TABLE]
By making use of the above inequalities, let us find an upper bound for each of the quantities , and . We begin with
[TABLE]
Next, we obtain
[TABLE]
Finally, for all ,
[TABLE]
Using these bounds, it clear that for all one has . On the other hand, a direct computation yields that for . Hence is univalent in , where for . From the above proof technique it is apparent that , where . That is, for , we have .
However, geometric properties of convex harmonic mappings gives a way to improve the lower bounds of . From Theorem , it is clear that is univalent and convex in the direction of . As univalent functions convex in one direction are close-to-convex in , it is clear that is close-to-convex in for every . From a classical result on convolution of analytic functions [6, Theorem 8.7, p. 248], it is clear that the radius of close-to-convexity of is greater than or equal to the radius of convexity of , where . From [6, Corollary 3, p. 256], it is clear that the radius of univalence of cannot exceed the radius of convexity of . The radius of convexity of is known to be for .
But then, from a result of Clunie and Sheil-Small [5, Lemma 5.15], we get that
[TABLE]
is univalent and close-to-convex in the disk for all .
Corollary 2**.**
Let satisfy the hypothesis of Theorem 2. Then is univalent in the disk
- (i)
, whenever ,
- (ii)
, whenever ,
- (ii)
, whenever .
Proof. The proof of Case (i) follows from Lemma and the result of Szegö [24]. The rest of the cases follows from Theorem 2. ∎
Acknowledgements
The research was supported by the project RUS/RFBR/P-163 under Department of Science & Technology (India) and the Russian Foundation for Basic Research (project 14-01-92692). The first author is currently on leave from Indian Institute of Technology Madras.
The reference list from the paper itself. Each links out to its DOI / PubMed record.
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- 2[2] I. E. Bazilevich, The problem of coefficients of univalent functions , Math. J. of the Aviation Institute (Moscow), (1945), 29–47.
- 3[3] L. de Branges, A proof of the Bieberbach conjecture , Acta Math. 154 (1-2)(1985), 137–152.
- 4[4] D. Bshouty, and W. Hengartner, Criteria for the extremality of the Koebe mapping , Proc. Amer. Math. Soc. 111 (1991), 403–411.
- 5[5] J. G. Clunie and T. Sheil-Small, Harmonic univalent functions , Ann. Acad. Sci. Fenn. Ser. A.I. 9 (1984), 3–25.
- 6[6] P. Duren, Univalent functions (Grundlehren der mathematischen Wissenschaften 259 , New York, Berlin, Heidelberg, Tokyo), Springer-Verlag, 1983.
- 7[7] P. Duren, Harmonic mappings in the plane, Cambridge Tracts in Mathematics, 156 , Cambridge Univ. Press, Cambridge, 2004.
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