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https://doi.org/10.1007/s40840-021-01122-x

Sharp Bounds of the Hermitian Toeplitz Determinants for Some Classes of Close-to-Convex Functions

Adam Lecko1 ·Barbara ´Smiarowska1

Received: 26 January 2021 / Revised: 17 March 2021 / Accepted: 5 April 2021 / Published online: 16 April 2021

© The Author(s) 2021

Abstract

Sharp upper and lower bounds of the Hermitian Toeplitz determinants of the second and third orders are found for various subclasses of close-to-convex functions.

Keywords Hermitian Toeplitz determinant·Univalent function·Close-to-convex functions·Carathéodory class

Mathematics Subject Classification 30C45·30C50

1 Introduction and Definitions

Let D := {z ∈ C : |z| < 1}andD := {z ∈ C : |z| ≤ 1},and forr > 0,let Tr := {z ∈ C : |z| = r}andT := T1. Denote byHbe the class of all analytic functions f inDand byAthe subclass ofHwith f normalized such that f(0)=0 and f(0)=1,so that f(z)is of the form

f(z)= n=1

anzn, a1:=1, z∈D. (1)

LetSbe the subclass ofAconsisting of univalent functions.

Communicated by V. Ravichandran.

B

Adam Lecko

alecko@matman.uwm.edu.pl Barbara ´Smiarowska

b.smiarowska@matman.uwm.edu.pl

1 Department of Complex Analysis, Faculty of Mathematics and Computer Science, University of Warmia and Mazury in Olsztyn, ul. Słoneczna 54, 10-710 Olsztyn, Poland

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Forq,n ∈N,consider the matrixTq,n(f)with fAgiven by (1) defined by

Tq,n(f):=

⎢⎢

⎢⎣

an an+1 . . .an+q1

an+1 an . . .an+q2

... ... ... ...

an+q1an+q2. . . an

⎥⎥

⎥⎦,

whereak :=ak.In the case whenanis a real number,Tq,n(f)is called an Hermitian Toeplitz matrix.

In recent years, a great many papers have been devoted to the estimation of deter- minants whose entries are coefficients of functions inA or its subclasses. Hankel matrices, i.e., square matrices which have constant entries along the reverse diagonal and the generalized Zalcman functional Jm,n(f):=am+n1aman, m,n∈N,are of particular interest (see, e.g., [5,6,8,13,15,16,18–20,25]). Also of interest are the determinants of symmetric Toeplitz matrices, the study of which was initiated in [1].

In [9,11,14], research was investigated into the study of Hermitian Toeplitz deter- minants whose entries are the coefficients of functions in subclasses ofA.

In this paper, we continue this research by computing the sharp upper and lower bounds of the second- and third-order Hermitian Toeplitz determinants over some subclasses of close-to-convex functions, but first noting that the following general result was proved in [11].

Theorem 1 ([11]) LetF be a subclass ofAsuch that{fF : a2 = 0} = ∅and A2(F):=max{|a2| : fF}exists. Then

1−A22(F)≤detT2,1(f)≤1.

Both inequalities are sharp.

We next define the classes of close-to-convex functions considered in this paper. First denote bySthe subclass ofSconsisting of the starlike functions, i.e., fSif and only if fAand

Rez f(z)

f(z) >0, z∈D.

A function fAis called close-to-convex if there existgSandδ ∈Rsuch that Reeiδz f(z)

g(z) >0, z∈D. (2)

The classCof all close-to-convex functions (which is necessarily a subclassS), was introduced by Kaplan [12] (see also [10, Vol. II, p. 3]), where the following geometrical interpretation was given:fAis close-to-convex if and only if there are no sections of the curve f(Tr),for everyr(0,1),in which tangent vector turns backward through an angle not less than π (cf. [10, Vol. II, p. 4]). Lewandowski [22,23] proved that

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the class of close-to-convex functions is identical with the class of linearly accessible functions introduced by Biernacki [3].

GivengSandδ∈R,letCδ(g)be the subclass ofCof all f satisfying (2). The four classesC0(gi),i =1, . . . ,4,where

g1(z):= z

1−z2, g2(z):= z

(1z)2, g3(z):= z 1+z+z2 and

g4(z):= z

1−z, z∈D,

are particularly interesting and have been studied by various authors (e.g., [2,7,17]). In [14], the sharp bounds of the second- and third-order Hermitian Toeplitz determinants were found for the classesC0(g1)andC0(g2).In this paper, we will do the same for the other two classes, i.e., forC0(g3)=:F1andC0(g4)=:F2which f in view of (2) satisfy the conditions

Re 1+z+z2

f(z)

>0, z∈D, (3)

and

Re

(1z)f(z)

>0, z∈D, (4)

respectively. We note here that in [21] the classesC(δ, ξ1, ξ2),whereδ(−π/2, π/2), ξ1, ξ2∈D,of univalent functions were introduced by generalizing Robertson’s con- dition for convexity in the direction of the imaginary axis [26]. In particular, the class C(0, (−1−√

3i)/2, (−1+√

3i)/2)is identical to the classF1and the classC(0,0,1) is identical to the classF2.A geometrical property of functions in classesC(δ, ξ1, ξ2) relating to the hyperbolic or parabolic family of arcs related toξ1andξ2was presented in [21].

LetPbe the class of allpHof the form p(z)=1+

n=1

cnzn, z∈D, (5)

having a positive real part inD.

2 Lemmas

In the proof of our main result, we will use the following lemma, see ([4], [24, p.

166]).

Lemma 1 If pPis of the form(5), then

|cn| ≤2, n ∈N. (6)

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Moreover,

c1=2ζ1 (7)

and

c2=2ζ12+2(1− |ζ1|22 (8) for someζi ∈D, i∈ {1,2}.

Forζ1∈T, there is a unique function p∈Pwith c1as in(7), namely p(z)= 1+ζ1z

1−ζ1z, z∈D.

Forζ1∈Dandζ2∈T, there is a unique function pP with c1and c2as in(7)and (8), namely

p(z)= 1+1ζ2+ζ1)z+ζ2z2

1+1ζ2ζ1)zζ2z2, z∈D. (9) 3 The ClassF1

Let fF1be the form (1). Then by (3) there exists pP of the form (5) such that

1+z+z2

f(z)= p(z), z∈D. (10)

Substituting (1) and (5) into (10) and equating the coefficients, we obtain a2= 1

2(−1+c1) , a3=1

3(−c1+c2) . (11)

Hence, using (6) it follows that A2(F1)=3/2 with f1F1satisfying

1+z+z2

f1(z)=1−z

1+z, z∈D, i.e.,

f1(z)= z

0

1−ξ

1+2ξ+2ξ2+ξ3 =z−3

2z2+ · · · , z∈D.

Also f2F1such that

1+z+z2

f2(z)= 1

1−z, z∈D, i.e.,

f2(z)= z

0

1−ξ3 =z+1

4z4+ · · ·, z∈D, (12) serves as the extreme function, sincea2=0. Thus, Theorem1gives

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Theorem 2 If fF1, then

−5

4 ≤detT2,1(f)≤1. Both inequalities are sharp.

We now find the upper and lower bounds of detT3,1(f)in the classF1, first noting that

detT3,1(f)=

1 a2 a3

a2 1 a2

a3a2 1 =2 Re

a22a3

−2|a2|2− |a3|2+1. (13)

Theorem 3 If fF1,then

−1≤detT3,1(f)≤1. (14) Both inequalities are sharp.

Proof We first find the upper bound.

By (11) and (6), we see that|a2| ≤3/2 and|a3| ≤4/3.Since Re(a22a3)≤ |a2|2|a3|, it follows from (13) that

detT3,1(f)F(|a2|,|a3|) , (15) where

F(x,y):=2x2y−2x2y2+1, (x,y)∈[0,3/2]×[0,4/3].

Observe now that the point(1,1)is the unique solution in(0,3/2)×(0,4/3)of the system of equations

∂F

∂x =4x(y−1)=0,

∂F

∂y =2(x2y)=0.

However,

2F

∂x2(1,1)2F

∂y2(1,1)− ∂F

∂x∂y(1,1) 2

= −16<0, so(1,1)is a saddle point ofF.

We now considerFon the boundary of[0,3/2] × [0,4/3].

(1) On the sidex=0,

F(0,y)=1−y2≤1, 0≤y≤ 4 3.

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(2) On the sidex=3/2,

F 3

2,y

= −7 2 +9

2yy2F 3

2,4 3

= 13

18, 0≤ y≤ 4 3. (3) On the sidey=0,

F(x,0)=1−2x2≤1, 0≤x≤ 3 2. (4) On the sidey=4/3

F

x,4 3

= −7 9+2

3x2≤ 13

18, 0≤x≤ 3 2.

Therefore, the inequalityF(x,y)≤1 holds for all(x,y)∈ [0,3/2]×[0,4/3],which in view of (15) gives the upper bound.

For the lower bound, we substitute (7) and (8) into (11) to obtain a2=1

2(−1+2ζ1) , a3=1 3

−2ζ1+2ζ12+2

1− |ζ1|2 ζ2

withζi ∈D,i =1,2.Therefore, from (13) we have detT3,1(f)= 1

181+Ψ2) , (16)

where

Ψ1:=9−20|ζ1|2+16|ζ1|4−8(1− |ζ1|2)22|2 (17) and

Ψ2:=30 Reζ1+6 Re ζ12

−32|ζ1|2Reζ1−8

1− |ζ1|2 Re

ζ1ζ2

+6

1− |ζ1|2

Reζ2+8

1− |ζ1|2 Re

ζ12ζ2

.

We now consider various cases.

A.Suppose thatζ1ζ2 = 0.Thenζ1 =reiθ andζ2= seiψ withr,s(0,1]and θ, ψ∈ [0,2π).Then

Ψ2=Ψ3+Ψ4, (18)

where

Ψ3:=30rcosθ+6r2cos 2θ−32r3cosθ

= −6r2+30rcosθ−32r3cosθ+12r2cos2θ (19)

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and

Ψ4:= −8r s 1−r2

cos(θ−ψ)+6s 1−r2

cosψ+8r2s

1−r2

cos(2θ−ψ)

=2s(1−r2)

κ12+κ22sin+α),

(20) whereα∈Rsatisfies

cosα= κ1

κ12+κ22, sinα= κ2

κ12+κ22 (21)

with

κ1:= −4rsinθ+4r2sin 2θ, κ2:=3−4rcosθ+4r2cos 2θ. (22) Since sin(ψ+α)≥ −1 ands≤1, we have

Ψ4≥ −2

1−r2 κ12+κ22

= −2

1−r2 9−8r2+16r4−24rcosθ−32r3cosθ+48r2cos2θ.

Therefore, from (18)–(20), we obtain Ψ23+Ψ4

≥30rcosθ+6r2cos 2θ−32r3cosθ

−2

1−r2 9−8r2+16r4−24rcosθ−32r3cosθ+48r2cos2θ.

(23) Noting that|ζ2| ≤1 from (17) we have

Ψ1≥1−4r2+8r4. (24)

Thus, from (16), (23) and (24) it follows that

18 detT3,1(f)G(r,cosθ), r(0,1], θ∈ [0,2π), (25) where

G(t,x):=g1(t,x)−2(1−t2) g2(t,x) with

g1(t,x):=1−10t2+8t4+30t x−32t3x+12t2x2 and

g2(t,x):=9−8t2+16t4−24t x−32t3x+48t2x2 (26)

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fort ∈ [0,1]andx∈ [−1,1].

LetΩ:= [0,1] × [−1,1].Now we will show that min{G(t,x):(t,x)Ω} = −18.

A1.We next deal with the critical points ofG in the interior ofΩ, i.e., in(0,1)× (−1,1).Note thatg2(t,x)≥0.Moreover,g2(t,x)=0 holds only fort =√

3/2 and x=√

3/3. A1.1.Whent =√

3/2 andx=√

3/3,from (17), (19)and (20) we have Ψ1=3−1

2|ζ2|2, Ψ3= 3

2, Ψ4=0, which gives

detT3,1(f)= − 1

36(−9+ |ζ2|2)≥ 2 9.

A1.2.We now consider caseg2(t,x) >0.DifferentiatingGwith respect toxyields 0= ∂G

∂x(t,x)= ∂g1

∂x (t,x)(1t2)(g2(t,x))1/2∂g2

∂x(t,x). (27) A1.2.a.Assume first that∂g1/∂x =0.Then from (27), it follows that∂g2/∂x =0, which is possible only fort =√

6/2>1 andx=√ 6/4.

A1.2.b.Assume next that∂g1/∂x =0.Then we can write (27) as

g2(t,x)1/2=

1−t2∂g2

∂x (t,x)

∂g1

∂x(t,x) = 4

1−t2 −3−4t2+12t x

15−16t2+12t x , (28)

or equivalently, by substituting (26), as

Φ =Φ(t,x):=3840t8−12800t7x+24576t6x2−23040t5x3+6912t4x4

−9600t6+16128t5x−21888t4x2+13824t3x3+10112t4

−2784t3x+1152t2x2−6216t2−1008t x+1881=0.

(29) Now note that by (28) the inequality

0< (g2(t,x))1/2 4

1−t2 = −3−4t2+12t x

15−16t2+12t x (30)

holds for

0<t <

3

2 and 4t2+3

12t <x <16t2−15 12t .

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DifferentiatingGwith respect tot, we have

∂G

∂t (t,x)=∂g1

∂t (t,x)+4t(g2(t,x))1/2− 1−t2

(g2(t,x))1/2∂g2

∂t (t,x). (31) By (28) and (31), we get

∂G

∂t (t,x)= − 72t

12xt−4t2−3 12xt−16t2+15H(t,x),

where for(t,x)(0,1)×(−1,1), H(t,x):=

−3+4t2−4t x 9−18t2+8t4+6t x+8t3x−24t2x2 .

Therefore, each critical point ofGsatisfies

−3+4t2−4t x=0 (32) or

9−18t2+8t4+6t x+8t3x−24t2x2=0. (33) I.Assume that (32) holds, thenx = x(t)=(−3+4t2)/(4t).Thus, by (29) we see that

Φ

t,−3+4t2 4t

= −8(2t+1)(2t−1)

4t2−5 2t2−3 2

=0

occurs only whent=1/2.Thus,x=x(1/2)= −1.However, it can be seen that the right side of (30) equals to−2 fort =1/2 andx = −1,which means that then the inequality (30) is not true. Therefore,Gdoes not have critical point in the interior of Ωin the case of (32).

II.Suppose now that (33) is satisfied. Since Eq. (33) is a quadratic inxwith:=

225−408t2+208t4>0, t(0,1),it has two roots, namely xi =xi(t)= 3+4t2+(−1)i+1

225−408t2+208t4

24t , i =1,2. (34)

a.Letx=x1.ThenΦ(t,x1(t))=0 is equivalent to the equation

−561+2204t2−2736t4+1088t6 225−408t2+208t4

=11169−48552t2+80288t4−59520t6+16640t8. (35) Squaring both sides of (35) leads to

2304γ1(t)γ22(t)=0, (36)

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where fort(0,1),

γ1(t):=289−408t2+208t4 and

γ2(t):=9−27t2+26t4−8t6= −(1−t)(1+t)

3−4t2 3−2t2 .

We see that there is a unique roott =√

3/2 of the Eq. (36), which also satisfies (35).

Then by (34),x1(

3/2)=√

3/3.However, this case was discussed in A1.1.

b.Letx=x2.ThenΦ(t,x2(t))=0 is equivalent to the equation

−561+2204t2−2736t4+1088t6 225−408t2+208t4

=11169−48552t2+80288t4−59520t6+16640t8. (37) Squaring both sides of (37) yields again the Eq. (36) having a unique roott =√

3/2, which does not satisfy (37)

A2.It therefore remains to considerGon the boundary ofΩ. (1) On the sidet =0,

G(0,x)≡ −5, x∈ [−1,1].

(2) On the sidet =1,

G(1,x)= −1−2x+12x2G

1, 1 12

= −13

12, x ∈ [−1,1].

(3) On the sidex = −1,

G(t,−1)= −5−38t+40t3+16t4=:1(t), t∈ [0,1].

Since1(t)=0 occurs only whent=1/2 and1(1/2)=168>0, we have 1(t)1(1/2)= −18, t ∈ [0,1].

(4) On the sidex =1,

G(t,1)= −5+38t−40t3+16t4=:2(t), t ∈ [0,1].

Since 2(t) = 0 occurs only when t = (19−√

57)/16 ∈ [0,1] and2((19

√57)/16)=(57−27√

57)/2<0, we have

2(t)2(0)= −5, t ∈ [0,1].

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B.Suppose thatζ1=0.Then

Ψ1=9−8|ζ2|2, Ψ2=6 Reζ2, and therefore,

detT3,1(f)= 1

18(9+6 Reζ2−8|ζ2|2)≥ −5

18. (38)

C.Suppose thatζ2=0 andζ1=reiθ =0,wherer(0,1]andθ∈ [0,2π).Then Ψ1=9−20|ζ1|2+16|ζ1|4=9−20r2+16r4

and

Ψ2=30 Reζ1+6 Re ζ12

−32|ζ1|2Reζ1=30rcosθ+6r2cos 2θ−32r3cosθ.

Thus,

18 detT3,1(f)=G(r,cosθ), r(0,1], θ∈ [0,2π), where

G(t,x):=9−26t2+16t4+30t x−32t3x+12t2x2 fort(0,1]andx∈ [−1,1].Set

xw := −15−16t2

12t , t(0,1].

Note that−1<xw occurs fort > (

69−3)/8=0.663328· · · ,andxw<1 holds fort(0,1).Hence, fort

(

69−3)/8,1

we have G(t,x)G(t,xw)= −39

4 +14t2−16

3 t4=:φ1(t).

Sinceφ1is increasing in (

69−3)/8,1 ,so

φ1(t)≥ − 1 32

123+3√ 69

= −4.622495· · ·

for t(

69−3)/8,1

. Further, xw < −1 occurs fort ∈ 0, (√

69−3)/8 . Hence,

G(t,x)G(t,−1)=9−30t−14t2+32t3+16t4=:φ2(t).

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Sinceφ2(t)=0 have a unique roott0=(−2+√

19)/4=0.589724· · · andφ2(t0)= 152>0, then

φ2(t)φ2

1 4

−2+√ 19

= −81

16= −5.062500· · ·, t

0,1 8

√ 69−3

.

Summarizing, form Parts A–C it follows the lower bound in (14).

We discuss now sharpness of (14). The function f2 defined by (12), for which a2 = a3 = 0, is extremal for the upper bound in (14). It is observed from (16), (23), (24) and (25) that equality for the lower bound in (14) holds when the following conditions are satisfied:

r =1

2, cosθ= −1, s=1, sin(ψ+α)= −1, (39) whereαis determined by the condition (21) withκ1andκ2given in (22). Thus,θ=π, α=π/2 andψ =π.Consequently,ζ1= −1/2 andζ2= −1,which in view of (9) holds for the function

p(z)= 1−z2

1+z+z2, z∈D,

in the classP.Therefore, the extremal function f in the classF1for the lower bound in (14) satisfies (10) with p given as above, having the coefficientsa2 = −1 and

a3=0.

4 The ClassF2

Let fF2be the form (1). Then by (4) there exists pP of the form (5) such that

(1z)f(z)= p(z), z∈D. (40)

Putting the series (1) and (5) into (40) by equating the coefficients, we get a2= 1

2(1+c1), a3= 1

3(1+c1+c2). (41) Hence and by (6), it follows that A2(F2)=3/2 with the extremal function f1F2

such that

(1z)f1(z)= 1+z

1−z, z∈D. (42)

Observe also thata2=0 for the function f2F2such that (1z)f2(z)= 1

1+z, z∈D.

Therefore, by Theorem1we have

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Theorem 4 If fF2, then

−5

4 ≤detT2,1(f)≤1. Both inequalities are sharp.

Now we estimate detT3,1(f)for functions in the classF2. Theorem 5 If fF2,then

detT3,1(f)≤ 11

9 . (43)

The inequality is sharp.

Proof By (41) and (6), we see that|a2| ≤ 3/2 and|a3| ≤ 5/3.As in the proof of Theorem3, the inequality (15) holds with the function

F(x,y):=2x2y−2x2y2+1, (x,y)∈ [0,3/2] × [0,5/3].

Repeating argumentation in the proof of Theorem3, we see that the functionF does not have any relative maxima in(0,3/2)×(0,5/3).

We considerFon the boundary of[0,3/2] × [0,5/3].

(1) On the sidex=0,

F(0,y)=1−y2≤1, 0≤y≤ 5 3. (2) On the sidex=3/2,

F 3

2,y

= −7 2 +9

2yy2F 3

2,5 3

= 11

9 , 0≤ y≤ 5 3. (3) On the sidey=0,

F(x,0)=1−2x2≤1, 0≤x≤ 3 2. (4) On the sidey=5/3,

F

x,5 3

= −16 9 +4

3x2F 3

2,5 3

= 11

9 , 0≤x ≤ 3 2.

Therefore, the inequality F(x,y)≤ 11/9 holds for all(x,y) ∈ [0,3/2] × [0,5/3]

which in view of (15) shows (43).

For the function f1given by (42),a2 =3/2 anda3=5/3 which makes equality

in (43).

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Theorem 6 If fF2,then detT3,1(f)≥ 1

44

32−31√ 3

= −0.493035· · · (44)

The inequality is sharp.

Proof Substituting (7) and (8) into (41) yields a2=1

2(1+1) , a3= 1 3

1+2ζ1+2ζ12+2

1− |ζ1|2 ζ2

,

for someζi ∈D(i =1,2). Therefore, from (13) we get detT3,1(f)= 1

181+Ψ2) , (45)

where

Ψ1:=10−20|ζ1|2+16|ζ1|4−8

1− |ζ1|22

2|2 (46) and

Ψ2:= −26 Reζ1+10 Re ζ12

+32|ζ1|2Reζ1+8

1− |ζ1|2 Re

ζ1ζ2

−2

1− |ζ1|2

Reζ2+8(1− |ζ1|2)Re ζ12ζ2

.

A.Suppose thatζ1ζ2 = 0.Thus,ζ1 = reiθ andζ2 = seiψ withr,s(0,1] and θ, ψ∈ [0,2π).Then

Ψ2=23+Ψ4) , (47)

where

Ψ3:= −13rcosθ+5r2cos 2θ+16r3cosθ

= −5r2−13rcosθ+16r3cosθ+10r2cos2θ (48) and

Ψ4:=4r s

1−r2

cos(θ−ψ)s

1−r2

cosψ+4r2s

1−r2

cos(2θ−ψ)

=s

1−r2 κ12+κ22sin(ψ+α),

(49) whereαis the quantity satisfying (21) with

κ1:=4rsinθ+4r2sin 2θ, κ2:= −1+4rcosθ+4r2cos 2θ. (50) Since sin(ψ+α)≥ −1 ands≤1, we have

Ψ4≥ −

1−r2 κ12+κ22

= −

1−r2 1+24r2+16r4−8rcosθ+32r3cosθ−16r2cos2θ.

(15)

Therefore, from (47), (48) and (49), we get 1

2Ψ23+Ψ4

≥ −13rcosθ+5r2cos 2θ+16r3cosθ

1−r2 1+24r2+16r4−8rcosθ+32r3cosθ−16r2cos2θ.

(51) Taking into account that|ζ2| ≤1 from (46) we have

Ψ1≥2

1−2r2+4r4

. (52)

Thus, from (45), (51) and (52) it follows that

9 detT3,1(f)G(r,cosθ), r(0,1], θ∈ [0,2π), (53) where

G(t,x):=g1(t,x)

1−t2 g2(t,x) with

g1(t,x):=1−7t2+4t4−13t x+16t3x+10t2x2 and

g2(t,x):=1+24t2+16t4−8t x+32t3x−16t2x2 (54) fort ∈ [0,1]andx∈ [−1,1].

LetΩ:= [0,1] × [−1,1]and Θ:= 9

44

32−31√ 3

= −4.4373· · · .

Now we will show that

min{G(t,x):(t,x)Ω} =Θ.

A1. For this, we first we find the critical points of G in the interior ofΩ, i.e., in (0,1)×(−1,1).Sinceg2(t,x)= 0 holds only fort = (

2−1)/2 andx = 1,it follows thatg2(t,x) >0 for(t,x)(0,1)×(−1,1).

DifferentiatingGwith respect toxyields 0= ∂G

∂x(t,x)= ∂g1

∂x (t,x)−1

2(1t2)(g2(t,x))1/2∂g2

∂x (t,x). (55)

(16)

A1.1Assume first that∂g1/∂x=0.Then by (55), it follows that∂g2/∂x=0,which is possible only fort =√

2/2 andx=√

2/4.From (53), we have

9 detT3,1(f)G

2 2 ,

√2 4

= −17 8 −3

2

√2= −4.246320. . .

A1.2Assume now that∂g1/∂x=0.Then we can write the Eq. (55) as

g2(t,x)1/2=

1−t2∂g2

∂x(t,x) 2∂g1

∂x (t,x) =4

1−t2 −1+4t2−4t x

−13+16t2+20t x , (56)

or equivalently, by substituting (54), as

Φ =Φ(t,x):=3840t8+18944t7x+22528t6x2+2560t5x3−6400t4x4 +128t6−9472t5x−4992t4x2+5120t3x3−7552t4

−2336t3x+1600t2x2+3800t2−2000t x+153=0.

(57)

Furthermore, note that by (56) the inequality 0< (g2(t,x))1/2

4

1−t2 = −1+4t2−4t x

−13+16t2+20t x (58)

is true for

0<t <

√2

2 and 4t2−1

4t <x<13−16t2 20t

or √

2

2 <t <1 and

x< 4t2−1

4t or x>−16t2−13 20t

. DifferentiatingGwith respect totyields

∂G

∂t (t,x)=∂g1

∂t (t,x)+2t(g2(t,x))1/2−1 2

1−t2

(g2(t,x))1/2∂g2

∂t (t,x). (59) By (56) and (59), we get

∂G

∂t (t,x)= − 36t

−4xt+4t2−1 20xt+16t2−13H(t,x),

where

H(t,x):=

−3+4t2+4t x −11+6t2+8t4+2t x+24t3x+40t2x2 .

(17)

Therefore, each critical point ofGsatisfies

−3+4t2+4t x=0 (60) or

−11+6t2+8t4+2t x+24t3x+40t2x2=0. (61) I.Assume that (60) holds. Thenx=x(t)=(3−4t2)/(4t).Thus, by (57) we see that

Φ

t,3−4t2 4t

= −8(48t4−104t2+39)(2t2−1)2=0

occurs only whent = ˆti, i =1,2,where tˆ1:= 1

6

39−6√

13=0.6945· · · , tˆ2:=

√2

2 =0.7071· · · Thus,

x=xtˆ1

= ˆx1= −2+√ 13

39−6√

13 =0.3852· · · and

x=xtˆ2

= ˆx2=

√2

4 =0.3535· · · . However, it can be seen that

−1+4ˆt12−4tˆ1xˆ1

−13+16ˆt12+20ˆt1xˆ1

= −2<0,

which means that the inequality (58) is not satisfied fort = ˆt1andx= ˆx1. Note that the caset= ˆt2andx= ˆx2reduces to A1.1.

Therefore,Gdoes not have critical point in the interior ofΩ.

II.Suppose now that (61) is satisfied. Equation (61) as a quadratic equation ofxwith :=441−216t2−176t4>0, t(0,1)has two roots, namely

xi =xi(t)= −

1+12t2

+(−1)i+1

441−216t2−176t4

40t , i =1,2. (62)

a.Letx=x1.ThenΦ(t,x1(t))=0 is equivalent to the equation −603−940t2−9936t4+7104t6 441−216t2−176t4

= −2313−96696t2+20384t4−44928t6+92928t8. (63)

(18)

Squaring the both sides of (63) leads to

518400γ1(t)γ22(t)=0, (64) where fort(0,1),

γ1(t):= −299+648t2+528t4 and

γ2(t):=1+t2−10t4+8t6=(1t)(1+t)

1+4t2 1−2t2 .

Thus, there are two rootst1andt2in(0,1)of the Eq. (64), namely

t1:=

√2

2 =0.707· · ·, t2:= 1 66

−2673+2442√

3=0.59779· · · . (65) Fort =t1, by (62),x˜1:=x1(t1)=√

2/4 and this case was discussed in A1.1.

Fort =t2, by (62),

˜

x2:=x1(t2)= 21+13√ 3 2

−2673+2442√

3 =0.551477· · · . (66) It can be verified that(t˜ 2,x˜2) = 0 and the inequality (58) holds for t = t2 and x= ˜x2. Therefore,Ghas a critical point at(t2,x˜2).

b.Letx=x2.ThenΦ(t,x2(t))=0 is equivalent to the equation

−603−940t2−9936t4+7104t6 441−216t2−176t4

= −2313−96696t2+20384t4−44928t6+92928t8. (67) Squaring both sides of (67) yields again the Eq. (64) having rootst1andt2given by (65), which do not satisfy (67).

Therefore, by A, B1 and B2, the functionGhas a unique critical point at(t2,x˜2).

Denote

λ1:= 2G

∂t2 (t2,x˜2)= −30910188

351923 +90657386 1055769

√3=60.89649· · ·,

λ2:= 2G

∂t∂x(t2,x˜2)= −211055

1177 +396373 3531

√3,

λ3 = 2G

∂x2 (t2,x˜2)= −308371

1177 +551104 3531

√3.

(19)

Sinceλ1>0 and

λ1λ3λ22= −7933032

1177 +4769748 1177

√3=279.02623· · ·>0,

the functionGhas a local minimum at(t2,x˜2).

A2.It remains to considerGin the boundary of. (1) On the sidet =0,

G(0,x)≡0> , x∈ [−1,1].

(2) On the sidet =1,

G(1,x)= −2+3x+10x2G

1,−3 20

= −89

40 > , x∈ [−1,1].

(3) On the sidex = −1, G(t,−1)=t

9+8t−12t2

G(0,−1)=0> , t∈ [0,1].

(4) On the sidex =1,

G(t,1)=1−13t+3t2+16t3+4t4

1−t2 −1+4t+4t2=:(t).

Whent

0, (−1+√ 2)/2

=:I1, we have−1+4t+4t2≤0. Therefore,

(t)=t

−9+8t+12t2G

√ 2−1

2 ,1

= −√

2≈ −1.41421> , tI1.

When t

(−1+√ 2)/2,1

=: I2, we have −1+4t +4t2 ≥ 0 and (t) = (−2+t+2t2)(−1+8t+4t2). Since(t)=0 occurs only whent =1/2∈I2and (1/2)=80>0,we have

(t) 1

2

= −4> , tI2. B.Suppose thatζ1=0.Then

Ψ1=10−8|ζ2|2, Ψ2= −2 Re2) , and therefore,

detT3,1(f)= 1 18

10−8|ζ2|2−2 Re2)

≥0.

(20)

C.Suppose thatζ2=0 andζ1=0.Then

Ψ1=10−20|ζ1|2+16|ζ1|4, Ψ2= −26 Reζ1+10 Re(ζ12)+32|ζ1|2Reζ1. Thus, takingζ1=reiθ,wherer(0,1]andθ∈ [0,2π)we have

Ψ1=10−20r2+16r4 Ψ2= −26rcosθ+10r2cos 2θ+32r3cosθ.

Then

9 detT3,1(f)=G(r,cosθ), r(0,1], θ ∈ [0,2π), where

G(t,x):=5−15t2+8t4−13t x+16t3x+10t2x2 fort(0,1]andx∈ [−1,1].Set

xw =13−16t2

20t , t(0,1].

Note that−1<xw occurs fort(0,1)andxw <1 holds fort > (

77−5)/8= 0.471870· · · .Hence, fort

(

77−5)/8,1

we have G(t,x)G(t,xw)= 31

40−23 5 t2+8

5t4=:φ1(t).

Sinceφ1is decreasing in (

77−5)/8,1 ,

φ1(t)≥ −89

40 = −2.225, t ∈ 1

8 √

77−5 ,1

.

On the other hand,xw>1 occurs fort ∈ 0, (√

77−5)/8

.Hence, G(t,x)G(t,1)=5−13t−5t2+16t3+8t4=:φ2(t).

Sinceφ2is decreasing in(0, (

77−5)/8), φ2(t)≥ 33

64 − 5 64

√77= −0.169919· · · , t

0,1 8

√ 77−5

.

Summarizing, form Parts A–C it follows that the inequality (44) holds.

It remains to show that the inequality (44) is sharp. It is observed from (45), (51), (52) and (53) that 9 detT3,1(f)=holds when the following conditions are satisfied:

r =t2, cosθ = ˜x2, s=1, sin+α)= −1, (68)

(21)

wheret2andx˜2are given by (65) and (66), and whereαis determined by the condition (21) withκ1andκ2given by (50).

Now setθ = Arccos(x˜2)so that it satisfies the second condition in (68). Then κ1 =3.309903· · · >0 andκ2 = −0.241293· · · <0. Thus, (21) is satisfied if we take

α= −Arccos

κ1

κ12+κ22

⎠= −0.0727716· · · .

Thus, if we put

ψ= 3π

2 −α=4.7851606· · · ,

thenψsatisfies the fourth condition in (68). Now consider a functionp˜which has the form (9) withζ1 =t2eiθ andζ2 =eiψ. Sinceζ1 ∈Dandζ2∈ T, from Lemma1it follows that p˜∈P, and so the extremal function f in the classF2for which equality

in (44) holds satisfies (40) with p:= ˜p.

Acknowledgements The authors thank the reviewers for theirs constructive comments and suggestions that helped to improve the clarity of this manuscript.

Funding None.

Declarations

Conflict of interest The authors declare that they have no conflict of interests.

Open Access This article is licensed under a Creative Commons Attribution 4.0 International License, which permits use, sharing, adaptation, distribution and reproduction in any medium or format, as long as you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons licence, and indicate if changes were made. The images or other third party material in this article are included in the article’s Creative Commons licence, unless indicated otherwise in a credit line to the material. If material is not included in the article’s Creative Commons licence and your intended use is not permitted by statutory regulation or exceeds the permitted use, you will need to obtain permission directly from the copyright holder. To view a copy of this licence, visithttp://creativecommons.org/licenses/by/4.0/.

References

1. Ali, Md Firoz, Thomas, D.K., Vasudevarao, A.: Toeplitz determinants whose elements are the coeffi- cients of analytic and univalent functions. Bull. Austr. Math. Soc.97(2), 253–264 (2018)

2. Ali, M.F., Vasudevarao, A.: On logarithmic coefficients of some close-to-convex functions. Proc. Am.

Math. Soc.146, 1131–1142 (2018)

3. Biernacki, M.: Sur la représentation conforme des domaines linéairement accessibles. Prace Mat.-Fiz.

44, 293–314 (1936)

4. Carathéodory, C.: Über den Variabilitatsbereich der Koeffizienten von Potenzreihen, die gegebene werte nicht annehmen. Math. Ann.64, 95–115 (1907)

(22)

5. 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. Inequal.11(2), 429–439 (2017)

6. Cho, N.E., Kowalczyk, B., Kwon, O.S., Lecko, A., Sim, Y.J.: The bounds of some determinants for starlike functions of order alpha. Bull. Malays. Math. Sci. Soc.41(1), 523–535 (2018)

7. Cho, N.E., Kowalczyk, B., Kwon, O.S., Lecko, A., Sim, Y.J.: On the third logarithmic coefficient in some subclasses of close-to-convex functions. Rev. R. Acad. Cienc. Exactas Fís. Nat.114(52), 1–14 (2020)

8. 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.100, 86–96 (2019) 9. Cudna, K., Kwon, O.S., Lecko, A., Sim, Y.J., ´Smiarowska, B.: The second and third-order Hermitian

Toeplitz determinants for starlike and convex functions of orderα. Bol. Soc. Mat. Mex.26, 361–375 (2020)

10. Goodman, A.W.: Univalent Functions. Mariner, Tampa (1983)

11. Jastrz¸ebski, P., 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.

114(166), 1–14 (2020)

12. Kaplan, W.: Close to convex schlicht functions. Mich. Math. J.1, 169–185 (1952)

13. Kowalczyk, B., Kwon, O.S., Lecko, A., Sim, Y.J.: The bounds of some determinants for functions of bounded turning of order alpha. Bulletin de la Société Des Sciences et des Lettres de Łód´z: Recherches sur les déformationsLXVII(1), 107–118 (2017)

14. Kowalczyk, B., Kwon, O.S., Lecko, A., Sim, Y.J., ´Smiarowska, B.: The Third-Order Hermitian Toeplitz Determinant for Classes of Functions Convex in One Direction. Bull. Malays. Math. Sci. Soc.43, 3143–3158 (2020)

15. 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.97, 435–445 (2018)

16. Kowalczyk, B., Lecko, A., Lecko, M., Sim, Y.J.: The sharp bound of the third Hankel determinant for some classes of analytic functions. Bull. Korean Math. Soc.55(6), 1859–1868 (2018)

17. Kumar, U.P., Vasudevarao, A.: Logarithmic coefficients for certain subclasses of close-to-convex func- tions. Monatsh. Math.187, 543–563 (2018)

18. Kwon, O.S., Lecko, A., Sim, Y.J.: The bound of the Hankel determinant of the third kind for starlike functions. Bull. Malays. Math. Sci. Soc.42, 767–780 (2019)

19. Lecko, A., Sim, Y.J., ´Smiarowska, B.: The sharp bound of the Hankel determinant of the third kind for starlike functions of order 1/2. Complex Anal. Oper. Theory13, 2231–2238 (2019)

20. Lee, S.K., Ravichandran, V., Supramanian, S.: Bound for the second Hankel determinant of certain univalent functions. J. Inequal. Appl.2013(281), 1–17 (2013)

21. Lecko, A.: A generalization of analytic condition for convexity in one direction. Demonstr. Math.

XXX(1), 155–170 (2002)

22. Lewandowski, Z.: Sur l’identiteé de certaines classes de fonctions univalentes, I. Ann. Univ. Mariae Curie-Skłodowska Sect. A12, 131–146 (1958)

23. Lewandowski, Z.: Sur l’identiteé de certaines classes de fonctions univalentes, II. Ann. Univ. Mariae Curie-Skłodowska Sect. A14, 19–46 (1960)

24. Pommerenke, C.: Univalent Functions. Vandenhoeck & Ruprecht, Göttingen (1975)

25. Ravichandran, V., Verma, S.: Generalized Zalcman conjecture for some classes of analytic functions.

J. Math. Anal. Appl.450(1), 592–605 (2017)

26. Robertson, M.S.: Analytic functions star-like in one direction. Am. J. Math.58, 465–472 (1936)

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