Abstract
We consider the Toeplitz matrices whose elements are the coefficients of Bazilevič functions and obtain upper bounds for the first four determinants of these Toeplitz matrices. The results presented here are new and noble and the only prior compatible results are the recent publications by Thomas and Halim [1] for the classes of starlike and close-to-convex functions and Radhika et al. [2] for the class of functions with bounded boundary rotation.
1 Introduction
Let A denote the class of all functions f of the form
which are analytic in the open unit disk U = {z:|z| < 1} and let S denote the subclass of A consisting of univalent functions. Obviously, for functions f ∈ S we must have f′ ≠ 0, in U. For f ∈ S, we consider the family B(β) of Bazilevič functions of type β; 0 ≤ β ≤ 1 so that
The family B(β) of Bazilevič functions of type β; 0 ≤ β ≤ 1 provides a transition from the class of starlike functions to the class of functions of bounded boundary rotation. To see this, we note that for the choice of β = 0, we have B(β) ≡ S* (0) ≡ S*, the class of starlike functions f ∈ S so that R(zf′/f) > 0 in and for the choice of β = 1, we get the family R of functions f ∈ S of bounded boundary rotation so that R(f′) > 0 in U. (For further details see [3].)
Several authors (e.g. see [4-8]) have discussed various subfamilies of the well-known Bazilevič functions of type β from various viewpoints including their coefficient estimates. It is interesting to note in this connection that the earlier investigations on the subject do not seem to have made use of Toeplitz matrices and determinants. Toeplitz matrices are one of the well-studied classes of structured matrices. They arise in all branches of pure and applied mathematics, statistics and probability, image processing, quantum mechanics, queueing networks, signal processing and time series analysis, to name a few (e.g see Ye and Lim [9]). Toeplitz matrices have some of the most attractive computational properties and are amenable to a wide range of disparate algorithms and determinant computations.
Here we consider the symmetric Toeplitz determinant
and obtain upper bounds for the coefficient body Tq(n); q = 2,3; n = 1, 2, 3 where the entries of Tq(n) are the coefficients of functions of the form (1) that are in the family of Bazilevič functions B(β). As far as we are concerned, the results presented here are new and noble and the only prior compatible results are the recent publications by Thomas and Halim [1] for the classes of starlike and close-to-convex functions and Radhika et al. [2] for the class of functions with bounded boundary rotation. We shall need the following result [10] in order to prove our main theorems.
Lemma 1.1
Let
2 Coefficient estimates for Toeplitz determinant
In our first theorem we determine a sharp upper bound for the coefficient body T2(2).
Theorem 2.1
Let f given by (1) be in the classB(β); 0 ≤ β ≤ 1. Then we have the sharp bound
Proof
First note that by equating the corresponding coefficients in the equation
we obtain
In view of (2) and (3), a simple computation leads to
Note that, by Lemma 1.1, we may write 2p2 = p2 + x(4 − p2) where without loss of generality we let 0 ≤ p1 = p ≤ 2. Substituting this into the above equation we obtain the following quadratic equation in terms of x.
Using the triangle inequality we obtain
Differentiating Φ(p,β) with respect to p we obtain
Setting
But 2β3 − 4β2 − 14β − 8 < 0 for 0 ≤ β ≤ 1. Therefore, the maximum of
For p1=0, we have p2 = 2x. Therefore, from (4),
For p1=2 we have
The result is sharp for the functions given by
□
Remark 2.2
Theorem 2.1 for β = 0 yields the bound
In our next theorem, we determine an upper bound for the coefficient body T2(3).
Theorem 2.3
Let f given by (1), be in the class B(β), 0 ≤ β ≤ 1. Then
where
Proof
By equating the corresponding coefficients in the equation,
we obtain
In view of (6) and (7) and applying Lemma 1, denoting X = 4 − p2 and Y = (1 − |x|2)ζ, where 0 ≤ p ≤ 2 and |ζ| < 1 we get,
As in the proof of Theorem 1, without loss of generality, we can write p1 = p, where 0 ≤ p ≤ 2. Then an application of triangle inequality gives,
where
We need to find the maximum value of Ψ(p, |x|) on [0,2] × [0,1]. First, assume that there is a maximum at an interior point Ψ(p0, |x0|) of [0,2] × [0,1]. Differentiating Ψ(p, |x|) with respect to |x| and equating it to 0 implies that p = p0 = 2, which is a contradiction. Thus for the maximum of Ψ(p, |x|), we need only to consider the end points of [0,2] × [0,1].
For p = 0 we obtain
For p=2 we obtain
For |x|=0 we obtain
which has the maximum value |N1(β)p6 − N2(β)p4| on [0,2].
For |x| = 1 we obtain
which has the maximum values |64N1(β)−16N2(β)| for p = 2 and
Remark 2.4
Theorem 2 for β = 0 yields the bound |T2(3)| ≤ 7 for the class of starlike functions S* confirming the bound obtained by Thomas and Halim [1] and for β = 1 yields the bound |T2(3)| ≤ 4/9 for the class of functions with bounded boundary rotation R confirming the bound obtained by Radhika et al. [2].
Theorem 2.5
Let f given by (1) be in the class B(β), (0 ≤ β ≤ 1; β ≠ β0), then
where β0 ≈ 0.3676 is the positive root of the polynomial
and
Proof
Write
Using the same techniques as in Theorem 2, one can obtain with simple computations that
We need to show that
In view of (2), (3) and (7) and Lemma 1, where we denote X = 4 − p2 and Y = (1 − |x|2)ζ, where 0 ≤ p ≤ 2 and |ζ| < 1, one may easily get,
Applying the triangle inequality and assuming that p1 = p, where 0 ≤ p ≤ 2 we obtain
We need to find the maximum value of Ω(p,|x|) on [0,2] × [0,1]. First, assume that there is a maximum at an interior point Ω(p0,|x0|) of [0,2] × [0,1]. Differentiating Ω([,|x|) with respect to |x| and equating it to zero implies that p = p0 = 2, which is a contradiction. Thus for the maximum of Ω(p,|x|), we need only to consider the end points of [0,2] × [0,1].
For p = 0 we obtain
For p = 2 we obtain
For |x| = 0 we obtain
which has maximum value Ω(p,0) = M2(β) attained at the end point p = 2.
For |x| = 1 we obtain
which has maximum value
Thus
For the case β = β0, we compute |a2−a4| as follows
Since, each |pi| ≤ 2, an application of triangle inequality shows that
Therefore
This completes the proof of Theorem 2.5. □
Remark 2.6
Theorem 2.5 for β = 0 yields the bound |T3(2)| ≤ 8 for the class of starlike functions S* confirming the bound obtained by Thomas and Halim [1] and for β = 1 yields the bound |T3(2)| ≤ 4/9 for the class of functions with bounded boundary rotation R confirming the bound obtained by Radhika et al. [2].
Theorem 2.7
Let f given by (1), be in the class B(β), 0 ≤ β ≤ 1. Then
where
Proof
Expanding the determinant by using equations (2) and (3) and applying Lemma 1.1, we have
Without loss of generality, we let 0 ≤ p1 = p ≤ 2. Now substituting this into the above equation and applying the triangle inequality we obtain the following quadratic equation in terms of x.
Differentiating Γ(p, β) with respect to p we obtain
Setting ∂(Γ(p,β))/∂p = 0 yields either p = 0 or
But −4β3 − 13β2 − 14β − 15 < 0 for 0 ≤ β ≤ 1. Therefore, the maximum of |T3(1)| is attained at the end points p1 = p ∈ [0,2].
For p1 = 0 we have a2 = 0 and
For p1 = 2 we obtain
where
This completes the proof of Theorem 2.7. □
Remark 2.8
Theorem 2.5 for β = 0 yields the bound |T3(1)| ≤ 8 for the class of starlike functions S* confirming the bound obtained by Thomas and Halim [1] and for β = 1 yields the bound |T3(1)| ≤ 13/9 for the class of functions with bounded boundary rotation R confirming the bound obtained by Radhika et al. [2].
Conflict of interest
The authors declare that there is no conflict of interests regarding the publication of this paper.
Acknowledgement
The authors sincerely thank the referees for their insightful suggestions. The work of the third author is supported by a grant from Department of Science and Technology, Government of India vide ref: SR/FTP/MS-022/2012 under fast track scheme.
References
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© 2018 Radhika et al., published by De Gruyter
This work is licensed under the Creative Commons Attribution-NonCommercial-NoDerivatives 4.0 License.
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