Next Article in Journal
A Subclass of Multivalent Janowski Type q-Starlike Functions and Its Consequences
Next Article in Special Issue
Entropy-Like Properties and Lq-Norms of Hypergeometric Orthogonal Polynomials: Degree Asymptotics
Previous Article in Journal
Investigation of the Thermal QCD Matter from Canonical Sectors
Previous Article in Special Issue
Ordered Structures of Polynomials over Max-Plus Algebra
 
 
Font Type:
Arial Georgia Verdana
Font Size:
Aa Aa Aa
Line Spacing:
Column Width:
Background:
Article

The Third-Order Hermitian Toeplitz Determinant for Alpha-Convex Functions

Department of Complex Analysis, Faculty of Mathematics and Computer Science, University of Warmia and Mazury in Olsztyn, Ul. Słoneczna 54, 10-710 Olsztyn, Poland
Submission received: 24 June 2021 / Revised: 14 July 2021 / Accepted: 15 July 2021 / Published: 16 July 2021
(This article belongs to the Special Issue Special Functions and Polynomials)

Abstract

:
Sharp lower and upper bounds of the second- and third-order Hermitian Toeplitz determinants for the class of α -convex functions were found. The symmetry properties of the arithmetic mean underlying the definition of α -convexity and the symmetry properties of Hermitian matrices were used.

1. Introduction

Let be the class of all analytic functions in D : = { z C : | z | < 1 } and A be its subclass of functions f of the form:
f ( z ) = n = 1 a n z n , a 1 = 1 , z D .
Let S be the subclass of A of all univalent functions.
For α [ 0 , 1 ] , let M α denote the subclass of A of all functions f satisfying the condition:
Re { ( 1 α ) z f ( z ) f ( z ) + α ( 1 + z f ( z ) f ( z ) ) } > 0 , z D
The class M α was introduced by Mocanu [1] and its elements are called α -convex (see also [2] [Volume I, pp. 142–147]). For α = 0 , the condition (2) describes the class of starlike functions denoted by S * introduced by Alexander [3] ([4], as can also be seen in [2] [Volume I, Chapter 8]). For α = 1 , the condition (2) specifies the class of convex functions denoted by S c defined by the study [5] (see also [2] [Volume I, Chapter 8]). Thus, the classes M α create a “continuous passage” on α [ 0 , 1 ] from the set of convex functions M 1 to the set of starlike functions M 0 . One can see that the range of α can be extended to the real axis as well to the complex plane. In [1], Mocanu presented a geometrical interpretation of functions in the class M α . In [6], it was observed that M α M 0 for every α [ 0 , 1 ] . This result can be found in the paper due to Sakaguchi [7] that was published before the advent of the α -convexity concept (cf. [2] [Volume I. pp. 142–143]). Furthermore, in [6], the authors have shown that M α 1 M α 2 for every 0 α 2 α 1 1 . The class M α plays an important role in the geometric function theory and was studied by various authors (e.g., [8,9] [Chapter 7] with further references).
For q , n N , by T q , n ( f ) , with f A of the form (1), define the matrix:
T q , n ( f ) : = a n a n + 1 a n + q 1 a ¯ n + 1 a n a n + q 2 a ¯ n + q 1 a ¯ n + q 2 a n ,
where a ¯ k : = a k ¯ . In case, a n is a real number, T q , n ( f ) is the Hermitian Toeplitz matrix. Thus, the matrix T q , 1 ( f ) is like this. In particular:
det T 3 , 1 ( f ) = 1 a 2 a 3 a ¯ 2 1 a 2 a ¯ 3 a ¯ 2 1 = 1 + 2 Re ( a 2 2 a ¯ 3 ) 2 | a 2 | 2 | a 3 | 2 .
In recent years, many papers have been devoted to the estimation of determinants whose entries are coefficients of functions in the class A or its subclasses. Hankel matrices, i.e., square matrices which have constant entries along the reverse diagonal (see, e.g., [10,11,12], with further references), and the symmetric Toeplitz matrices (see [13]), are of particular interest.
For this reason, considering the interest of specialists, in [14,15,16], the estimation of the determinants of the Hermitian Toeplitz matrices T q , 1 ( f ) on the class A or its subclasses was started. Hermitian Toeplitz matrices play an important role in functional analysis, applied mathematics as well as in physics and technical sciences. Let us mention that only a few papers have been published that concern the estimation of Hermitian Toeplitz determinants in the basic subclasses of univalent functions. This is a new issue and it is important to find such estimates for the class of α -convex functions, which are among the most important in geometric function theory. This paper was dedicated to finding the sharp lower and upper bounds of the second- and third-order Hermitian Toeplitz determinants for the class M α .
Let 𝒫 be the class of all p of the form:
p ( z ) = 1 + n = 1 c n z n , z D ,
which have a positive real part.
In the proof of the main result, we will use the following lemma which contains the Carathéodory result for c 1 [17], and the well-known formula for c 2 (e.g., [18] [p. 166]).
Lemma 1. 
If p 𝒫 is of the form (4), then:
c 1 = 2 ζ 1 ,
and:
c 2 = 2 ζ 1 2 + 2 ( 1 | ζ 1 | 2 ) ζ 2
for some ζ 1 , ζ 2 D ¯ .
Observe that for each θ R , det T q , 1 ( f ) = det T q , 1 ( f θ ) , where f θ ( z ) : = e i θ f ( e i θ z ) , z D , i.e., det T q , 1 ( f ) is rotationally invariant.
Recall now the following observation [15].
Theorem 1. 
Let F be a subclass of A such that { f F : a 2 = 0 } and A 2 ( F ) : = max { | a 2 | : f F } exists. Then:
1 A 2 2 ( F ) det T 2 , 1 ( f ) 1 .
Both inequalities are sharp.

2. Main Results

We now compute the sharp bounds of det T 2 , 1 ( f ) and det T 3 , 1 ( f ) in the class of α -convex functions.
Let α [ 0 , 1 ] . In view of (11), we see that A 2 ( M α ) = 2 / ( α + 1 ) with the extremal function f M α satisfying:
( 1 α ) z f ( z ) f ( z ) + α 1 + z f ( z ) f ( z ) = 1 + z 1 z , z D ,
i.e., for α ( 0 , 1 ] , with the function:
f ( z ) = 1 α 0 z ζ 1 α 1 ( 1 ζ ) 2 α d ζ α , z D ,
called α -convex Koebe function, and for α = 0 with the Koebe function:
f ( z ) = z ( 1 z ) 2 , z D .
Hence, and by observing that the identity function belongs to the class M α , by Theorem 1, we have:
Theorem 2. 
Let α [ 0 , 1 ] . If f M α , then:
( 3 + α ) ( 1 α ) ( 1 + α ) 2 det T 2 , 1 ( f ) 1 .
Both inequalities are sharp.
Particularly, for α = 0 and α = 1 , i.e., for starlike and convex functions, we have the following result [14].
Corollary 1. 
  • If f S * , then:
    3 det T 2 , 1 ( f ) 1 .
  • If f S c , then:
    0 det T 2 , 1 ( f ) 1 .
All inequalities are sharp.
Now, we will compute the upper and lower bounds of det T 3 , 1 ( f ) .
Theorem 3. 
Let α [ 0 , 1 ] . If f M α , then:
det T 3 , 1 ( f ) 4 ( α 2 + 3 α + 1 ) ( α 2 + 4 α + 2 ) ( α 1 ) 2 ( α + 1 ) 4 ( 2 α + 1 ) 2 , 0 α < α 0 , 1 , α 0 α 1 ,
where α 0 = 0.404744 is the unique root in ( 0 , 1 ) of the equation:
33 α 4 + 96 α 3 + 38 α 2 16 α 7 = 0 ,
and:
det T 3 , 1 ( f ) ( α + 2 ) 2 ( α 1 ) 2 ( α 2 + 5 α + 2 ) ( α 2 + 3 α + 2 ) .
All inequalities are sharp.
Proof. 
Fix α [ 0 , 1 ] and let f M α be of the form (1). Then, by (2):
( 1 α ) z f ( z ) f ( z ) + α 1 + z f ( z ) f ( z ) = p ( z ) , z D ,
for a certain p 𝒫 of the form (4). Substituting the series (1) and (4) into (10), by equating the corresponding coefficients, we obtain:
a 2 = c 1 α + 1 , a 3 = ( α + 1 ) 2 c 2 + ( 3 α + 1 ) c 1 2 2 ( α + 1 ) 2 ( 2 α + 1 ) .
Since the class M α and the determinant det T 3 , 1 are rotationally invariant, by (5), we may assume that c 1 [ 0 , 2 ] , i.e., that ζ 1 [ 0 , 1 ] . Furthermore, (3) with (11), (5) and (6) give:
det T 3 , 1 ( f ) = 1 ( α + 1 ) 4 ( 2 α + 1 ) 2 × ( α 2 + 8 α + 3 ) ( α 2 8 α 5 ) ζ 1 4 8 ( 2 α + 1 ) 2 ( α + 1 ) 2 ζ 1 2 + ( α + 1 ) 4 ( 2 α + 1 ) 2 + 2 ( α + 1 ) 3 ( 1 α ) ζ 1 2 ( 1 ζ 1 2 ) Re ( ζ 2 ) ( α + 1 ) 4 ( 1 ζ 1 2 ) 2 | ζ 2 | 2
for some ζ 1 , ζ 2 D ¯ .
Define:
F ( x , y , t ) : = ( α 2 + 8 α + 3 ) ( α 2 8 α 5 ) x 2 8 ( 2 α + 1 ) 2 ( α + 1 ) 2 x + ( α + 1 ) 4 ( 2 α + 1 ) 2 + 2 ( α + 1 ) 3 ( 1 α ) ( 1 x ) x y cos t ( α + 1 ) 4 ( 1 x ) 2 y 2
for x , y [ 0 , 1 ] and t [ 0 , 2 π ] .
If ζ 2 0 , then ζ 2 = | ζ 2 | e i θ for a unique θ [ 0 , 2 π ) . Thus, by (12):
( α + 1 ) 4 ( 2 α + 1 ) 2 det T 3 , 1 ( f ) = F ( ζ 1 2 , | ζ 2 | , θ ) .
If ζ 2 = 0 , then by (12):
( α + 1 ) 4 ( 2 α + 1 ) 2 det T 3 , 1 ( f ) = F ( ζ 1 2 , 0 , θ ) = F ( ζ 1 2 , 0 , 0 ) .
Therefore, we will find the maximum and minimum value of F .
A. First, we show the inequality (8). We have:
F ( x , y , t ) F ( x , y , 0 ) = ( α 2 + 8 α + 3 ) ( α 2 8 α 5 ) x 2 8 ( 2 α + 1 ) 2 ( α + 1 ) 2 x + ( α + 1 ) 4 ( 2 α + 1 ) 2 + 2 ( α + 1 ) 3 ( 1 α ) ( 1 x ) x y ( α + 1 ) 4 ( 1 x ) 2 y 2 = : G ( x , y )
for x , y [ 0 , 1 ] and t [ 0 , 2 π ] .
A1. For x = 1 :
G ( 1 , y ) = 4 ( α 1 ) 2 ( α 2 + 3 α + 1 ) ( α 2 + 4 α + 2 ) , y [ 0 , 1 ] .
A2. Let x [ 0 , 1 ) . Set:
y w : = ( 1 α ) x ( 1 + α ) ( 1 x ) , x [ 0 , 1 ) .
(a) Note that y w = 0 if and only if α = 1 . Then, by (15) with α = 1 we obtain:
F ( x , y w , 0 ) = F ( x , 0 , 0 ) = 144 ( x 1 ) 2 144 , x [ 0 , 1 ) .
(b) Assume now that α [ 0 , 1 ) .
Observe that y w > 1 if and only if ( 1 + α ) / 2 < x < 1 . Then:
G ( x , y ) G ( x , 1 ) = 4 ( 5 α + 3 ) ( 3 α + 1 ) x 2 4 ( 8 α 2 + 7 α + 1 ) ( α + 1 ) 2 x + 4 α ( α + 1 ) 5 max G α + 1 2 , 1 , G ( 1 , 1 ) = max ( α 1 ) 2 ( 2 α + 1 ) 2 ( α + 1 ) 2 , 4 ( α 2 + 3 α + 1 ) ( α 2 + 4 α + 2 ) ( α 1 ) 2
for x [ 0 , 1 ) . Since the inequality:
( 1 α ) 2 ( 1 + 2 α ) 2 ( 1 + α ) 2 4 ( 1 α ) 2 ( α 2 + 3 α + 1 ) ( α 2 + 4 α + 2 )
is equivalent to:
( 1 α ) 2 ( 16 α 3 + 47 α 2 + 34 α + 7 ) 0 ,
which holds for α [ 0 , 1 ) , we deduce that:
G ( x , 1 ) G ( 1 , 1 ) = 4 ( α 1 ) 2 ( α 2 + 3 α + 1 ) ( α 2 + 4 α + 2 ) , 1 2 ( 1 + α ) < x < 1 .
Now, we consider the case y w 1 which holds only for 0 x ( α + 1 ) / 2 . Then:
G ( x , y ) G ( x , y w ) = 16 ( 2 α + 1 ) 2 x 2 8 ( 2 α + 1 ) 2 ( α + 1 ) 2 x + ( α + 1 ) 4 ( 2 α + 1 ) 2 max G 0 , y w , G α + 1 2 , y w = max ( α + 1 ) 4 ( 2 α + 1 ) 2 , ( α 1 ) 2 ( 2 α + 1 ) 2 ( α + 1 ) 2
for 0 x ( α + 1 ) / 2 . Since the inequality:
( α + 1 ) 4 ( 2 α + 1 ) 2 ( α 1 ) 2 ( 2 α + 1 ) 2 ( α + 1 ) 2
is equivalent to:
α ( 2 α 2 + 3 α + 1 ) 2 0 ,
which holds for α [ 0 , 1 ) , we deduce that:
G ( x , y w ) G ( 0 , y w ) = ( α + 1 ) 4 ( 2 α + 1 ) 2 , 0 x 1 2 ( α + 1 ) .
A3. Comparing (16), (18) and (19) with α [ 0 , 1 ) , leads to the inequality:
4 ( α 1 ) 2 ( α 2 + 3 α + 1 ) ( α 2 + 4 α + 2 ) ( α + 1 ) 4 ( 2 α + 1 ) 2
equivalently written:
33 α 4 96 α 3 38 α 2 + 16 α + 7 0 ,
which holds for α [ 0 , α 0 ] , where α 0 = 0.404744 Hence, by (13)–(15), (17), we obtain (8).
B. Now, we show the inequality (9). We have:
F ( x , y , t ) F ( x , y , π ) = ( α 2 + 8 α + 3 ) ( α 2 8 α 5 ) x 2 8 ( 2 α + 1 ) 2 ( α + 1 ) 2 x + ( α + 1 ) 4 ( 2 α + 1 ) 2 2 ( α + 1 ) 3 ( 1 α ) ( 1 x ) x y ( α + 1 ) 4 ( 1 x ) 2 y 2 = : H ( x , y )
for x , y [ 0 , 1 ] and t [ 0 , 2 π ] .
B1. For x = 1 :
H ( 1 , y ) = 4 α 6 + 20 α 5 + 8 α 4 52 α 3 12 α 2 + 24 α + 8 = 4 ( α 2 + 3 α + 1 ) ( α 2 + 4 α + 2 ) ( α 1 ) 2 0 , y [ 0 , 1 ] .
B2. Let x [ 0 , 1 ) . Set:
y w : = ( 1 α ) x ( α + 1 ) ( 1 x ) .
Since y w 0 , we have:
H ( x , y ) H ( x , 1 ) = 4 ( α 2 + 5 α + 2 ) ( α 2 + 3 α + 2 ) x 2 4 ( 7 α 2 + 7 α + 2 ) ( α + 1 ) 2 x + 4 α ( α + 1 ) 5 , x [ 0 , 1 ) .
For α [ 0 , 1 ] , let:
x w : = ( 7 α 2 + 7 α + 2 ) ( α + 1 ) 2 2 ( α 2 + 5 α + 2 ) ( α 2 + 3 α + 2 ) .
We see that x w > 0 , and x w 1 if and only if:
( 1 α ) ( α 2 + 5 α + 2 ) ( α 2 + 3 α + 2 ) ( 9 α 3 + 34 α 2 + 27 α + 6 ) 0 ,
which holds for α [ 0 , 1 ) . Therefore:
H ( x , 1 ) H ( x w , 1 ) = ( α 1 ) 2 ( 2 α + 1 ) 2 ( α + 2 ) 2 ( α + 1 ) 4 ( α 2 + 5 α + 2 ) ( α 2 + 3 α + 2 )
for x [ 0 , 1 ) .
B3. Comparing (21) and (23) from (20), (13) and (14), the inequality (9) is obtained.
C. It remains to show the sharpness of all results. The first inequality in (8) is sharp for the function f M α given by (7) for which by (11),
a 2 = 2 α + 1 , a 3 = ( α + 1 ) 2 + 2 ( 3 α + 1 ) ( α + 1 ) 2 ( 2 α + 1 ) .
The identity function is extremal for the second inequality in (8).
Set τ : = x w , where x w is given by (22). Since, as was noticed in B2, 0 < x w 1 for α [ 0 , 1 ] , the function:
p ˜ ( z ) : = 1 z 2 1 2 τ z + z 2 = 1 + 2 τ z + ( 4 τ 2 2 ) z 2 + , z D ,
belongs to 𝒫. Thus, the function f given by (10), with p : = p ˜ , being of the form (1) with:
a 2 = 2 τ α + 1 , a 3 = 2 ( α 2 + 5 α + 2 ) τ 2 ( 1 + α ) 2 ( α + 1 ) 2 ( 2 α + 1 )
belongs to M α and is extremal for the inequality (9). □
Particularly, for α = 0 and α = 1 we obtain the following result [14].
Corollary 2. 
  • If f S * , then:
    1 det T 3 , 1 ( f ) 8 .
  • If f S c , then:
    0 det T 3 , 1 ( f ) 1 .
All inequalities are sharp.

Funding

This research received no external funding.

Institutional Review Board Statement

Not applicable.

Informed Consent Statement

Not applicable.

Data Availability Statement

Not applicable.

Conflicts of Interest

The author declares no conflict of interest.

References

  1. Mocanu, P.T. Une propriété de convexité généralisé dans la théorie de la représentation conforme. Mathematica 1969, 11, 127–133. [Google Scholar]
  2. Goodman, A.W. Univalent Functions; Mariner: Tampa, FL, USA, 1983. [Google Scholar]
  3. Alexander, J.W. Functions which map the interior of the unit circle upon simple regions. Ann. Math. 1915, 17, 12–22. [Google Scholar] [CrossRef]
  4. Nevanlinna, R. Über die konforme Abbildung von Sterngebieten. Finska Vetenskaps-Societetens Förhandinger 1921, 53, 1–21. [Google Scholar]
  5. Study, E. Vorlesungen über ausgewählte Gegenstände der Geometrie, Zweites Heft; Konforme Abbildung Einfach-Zusammenhängender Bereiche; Druck: Leipzig, Germany; Verlag von B.G. Teubner: Berlin, Germany, 1913. [Google Scholar]
  6. Miller, S.S.; Mocanu, P.T.; Reade, M.O. All α-convex functions are univalent and starlike. Proc. Am. Math. Soc. 1973, 37, 553–554. [Google Scholar] [CrossRef]
  7. Sakaguchi, K. A note on p-valent functions. J. Math. Soc. Jpn. 1962, 14, 312–321. [Google Scholar] [CrossRef]
  8. Thomas, D.K.; Tuneski, N.; Vasudevarao, A. Univalent Functions. A Primer; De Gruyter Studies in Mathematics; De Gruyter: Berlin, Germany, 2018; Volume 69. [Google Scholar]
  9. Ravichandran, V.; Darus, M. On a class of α-convex functions. J. Anal. Appl. 2004, 2, 17–25. [Google Scholar]
  10. Cho, N.E.; Kowalczyk, B.; Kwon, O.S.; Lecko, A.; Sim, Y.J. Some coefficient inequalities related to the Hankel determinant for strongly starlike functions of order alpha. J. Math. Ineq. 2017, 11, 429–439. [Google Scholar] [CrossRef]
  11. Cho, N.E.; Kowalczyk, B.; Lecko, A. Sharp bounds of some coefficient functionals over the class of functions convex in the direction of the imaginary axis. Bull. Aust. Math. Soc. 2019, 100, 86–96. [Google Scholar] [CrossRef]
  12. Kowalczyk, B.; Lecko, A.; Sim, Y.J. The sharp bound of the Hankel determinant of the third kind for convex functions. Bull. Aust. Math. Soc. 2018, 97, 435–445. [Google Scholar] [CrossRef]
  13. Ali, M.F.; Thomas, D.K.; Vasudevarao, A. Toeplitz determinants whose elements are the coefficients of analytic and univalent functions. Bull. Aust. Math. Soc. 2018, 97, 253–264. [Google Scholar] [CrossRef]
  14. 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 α. Bol. Soc. Mat. Mex. 2020, 26, 361–375. [Google Scholar] [CrossRef]
  15. Jastrzębski, P.J.; Kowalczyk, B.; Kwon, O.S.; Lecko, A.; Sim, Y.J. Hermitian Toeplitz determinants of the second and third-order for classes of close-to-star functions. Rev. R. Acad. Cienc. Exactas Fís. Nat. 2020, 114, 1–14. [Google Scholar]
  16. 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. 2020, 43, 3143–3158. [Google Scholar] [CrossRef]
  17. Carathéodory, C. Über den Variabilitatsbereich der Koeffizienten von Potenzreihen, die gegebene werte nicht annehmen. Math. Ann. 1907, 64, 95–115. [Google Scholar] [CrossRef] [Green Version]
  18. Pommerenke, C. Univalent Functions; Vandenhoeck & Ruprecht: Göttingen, Germany, 1975. [Google Scholar]
Publisher’s Note: MDPI stays neutral with regard to jurisdictional claims in published maps and institutional affiliations.

Share and Cite

MDPI and ACS Style

Dobosz, A. The Third-Order Hermitian Toeplitz Determinant for Alpha-Convex Functions. Symmetry 2021, 13, 1274. https://0-doi-org.brum.beds.ac.uk/10.3390/sym13071274

AMA Style

Dobosz A. The Third-Order Hermitian Toeplitz Determinant for Alpha-Convex Functions. Symmetry. 2021; 13(7):1274. https://0-doi-org.brum.beds.ac.uk/10.3390/sym13071274

Chicago/Turabian Style

Dobosz, Anna. 2021. "The Third-Order Hermitian Toeplitz Determinant for Alpha-Convex Functions" Symmetry 13, no. 7: 1274. https://0-doi-org.brum.beds.ac.uk/10.3390/sym13071274

Note that from the first issue of 2016, this journal uses article numbers instead of page numbers. See further details here.

Article Metrics

Back to TopTop