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Coefficient bounds for certain families of bi-Bazilevič and bi-Ozaki-close-to-convex functions

  • The aim of this work is to introduce two families, BΣ(;ϑ) and OΣ(ϰ;ϑ), of holomorphic and bi-univalent functions involving the Bazilevič functions and the Ozaki-close-to-convex functions, by using generalized telephone numbers. We determinate upper bounds on the Fekete-Szegö type inequalities and the initial Taylor-Maclaurin coefficients for functions in these families. We also highlight certain edge cases and implications for our findings.

    Citation: Muajebah Hidan, Abbas Kareem Wanas, Faiz Chaseb Khudher, Gangadharan Murugusundaramoorthy, Mohamed Abdalla. Coefficient bounds for certain families of bi-Bazilevič and bi-Ozaki-close-to-convex functions[J]. AIMS Mathematics, 2024, 9(4): 8134-8147. doi: 10.3934/math.2024395

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  • The aim of this work is to introduce two families, BΣ(;ϑ) and OΣ(ϰ;ϑ), of holomorphic and bi-univalent functions involving the Bazilevič functions and the Ozaki-close-to-convex functions, by using generalized telephone numbers. We determinate upper bounds on the Fekete-Szegö type inequalities and the initial Taylor-Maclaurin coefficients for functions in these families. We also highlight certain edge cases and implications for our findings.



    Indicate by A the family of holomorphic functions in the open unit disk U={zC:|z|<1} of the form

    f(z)=z+k2akzk. (1.1)

    The A subfamily of functions that are univalent in U is denoted by S.

    We denote by S, C, and K the families of functions that starlike, convex, and close-to-convex in U, respectively, and given as follows:

    A function fS is said to be starlike if

    (zf(z)f(z))>0,zU,

    a function fS is said to be convex if

    ((zf(z))f(z))>0,zU,

    and a function fS is said to be a close-to-convex functions if

    (zf(z)g(z))>0;gS,zU.

    Note that, CSK.

    The families of functions that are starlike of order (0<1)  and convex of order (0<1)  are denoted by S() and C(), respectively, and are given as follows:

    S()={fS:(zf(z)f(z))>,zU}

    and

    C()={fS:((zf(z))f(z))>,zU}.

    A well known subclass of S, named as class of Bazilevič function[36], is defined as:

    B()={fA:(z1f(z)(f(z))1)>0;zU;0}.

    For 0απ, Kaplan [25] defined a subfamily of A called close-to-convex functions, given as:

    K(α)={fA:(eiαzf(z)g(z))>0;gS zU}.

    In 1935, Ozaki [34] considered functions in A satisfying the condition

    (1+zf(z)f(z))>12,zU,

    whose members are known to be close-to-convex and therefore univalent.

    Lately, Kargar and Ebadian [26] considered the generalization of Ozaki's condition as the following:

    Definition 1.1. Let fA be locally univalent for zU and let 12ϰ1. A function f is called an Ozaki-close-to-convex function in U if

    (1+zf(z)f(z))>12ϰ,zU.

    We denote by F(ϰ) the family of all Ozaki-close-to-convex functions. It is clear that, for 12ϰ12, we have F(ϰ)KS.

    In U, a function fA is considered bi-univalent if f and f1 are both univalent functions. Denote by Σ all bi-univalent functions in U. We revisit a few functions in the family Σ from Srivastava et al.'s work [41]. We notice that the family Σ consists of

    z1z,log(1z)and12log(1+z1z)

    and so is not empty, however the Koebe function is not a member of Σ. Also, the functions zz22 and z1z2 are not bi-univalent. A very large number of works related to the class Σ have been presented in the recent papers (one may see [1,3,6,8,10,11,12,14,16,18,19,22,23,24,27,28,29,31,32,33,38,39,40,42,43,44,45,46,49,50,51]).

    The Littlewood-Paley conjecture (see [21]) that the coefficients of odd univalent functions are bounded by unity has been refuted by Fekete and Szegö, a fact widely recognized in the field of Geometric Function Theory (GFT). Consequently, given fS, we get the Fekete-Szegö problem |a3a22|. Many authors studied and deduced the Fekete-Szegö inequality for different families of functions (see [2,3,4,5,9,13,17,30,35,38,40,41,47,48,53]) in GFT.

    The recurrence relation quantifies traditional telephone numbers:

    X()=X(1)+(1)X(2),2.

    Initial conditions:

    X(0)=X(1)=1.

    For integers 0 and ς1, Wloch and Wolowiec-Musial [52] defined generalized telephone numbers X(ς,) by the recurrence relation:

    X(ς,)=ςX(ς,1)+(1)X(ς,2),

    with initial conditions

    X(ς,0)=1andX(ς,1)=ς.

    Bednarz and Wolowiec-Musial [7] recently examined the accessible generalization of phone numbers using the formula

    Xς()=Xς(1)+ς(1)Xς(2),

    where 2 and ς1 with initial conditions

    Xς(0)=Xς(1)=1.

    According to Deniz [17], who conducted this investigation very recently, Xς() has an exponential generating function

    e(r+ςr22)==0Xς()r!.

    As ς=1, classical phone numbers Xς()X() are evident.

    Now, we study the function

    ϑ(z)=e(z+ςz22)=1+z+(1+ς)z22+(1+3ς)z36+ (2.1)

    with its domain of definition as the open unit disk U. Note that the holomorphic function ϑ(z) in U, with a positive real part such that ϑ(0)=1,ϑ(0)>0, and ϑ maps U onto an area that is symmetric with respect to the real axis and starlike with respect to 1. Using the generalized telephone numbers, we now give the following subfamilies of holomorphic bi-Ozaki-close-to-convex and bi-Bazilevič functions.

    Definition 2.1. If a function fΣ satisfies the following subordinations, it belongs to the family BΣ(;ϑ):

    z1f(z)(f(z))1e(z+ςz22)=:ϑ(z)

    and

    w1g(w)(g(w))1e(w+ςw22)=:ϑ(w),

    where is non-negative integer, ς1, and g(w)=f1(w). $

    Remark 2.1. If we take =0 in Definition 2.1, the family BΣ(;ϑ) reduces to the family SΣ(ϑ), which was studied recently by Cotȋrlǎ and Wanas (see [15]).

    Definition 2.2. The family OΣ(ϰ;ϑ) contains all the functions fΣ if the next subordinations satisfy:

    2ϰ12ϰ+1+22ϰ+1(1+zf(z)f(z))e(z+ςz22)=:ϑ(z)

    and

    2ϰ12ϰ+1+22ϰ+1(1+wg(w)g(w))e(w+ςw22)=:ϑ(w),

    where 12ϰ1, ς1, and g(w)=f1(w). $

    Remark 2.2. If we take ϰ=12 in Definition 2.2, the family OΣ(ϰ;ϑ) reduces to the family CΣ(ϑ), which was introduced recently by Cotȋrlǎ and Wanas (see [15]).

    In the following sections we determine the upper bounds on the Fekete-Szegö type inequalities and the initial Taylor-Maclaurin coefficients for functions in these families in Definitions 2.1 and 2.2.

    We recall the following lemma where we obtain the upper bounds on the Fekete-Szegö type inequalities and the initial Taylor-Maclaurin coefficients for functions in fBΣ(;ϑ), where is non-negative integer.

    Lemma 3.1. ([20], p.41) Let hP be given by the following series:

    h(z)=1+c1z+c2z2+,wherezU

    then

    |cn|2,forallnN.

    Theorem 3.1. If f given by (1.1) is in the family BΣ(;ϑ), where is non-negative integer, then

    |a2|min{1+1,2|(+2)(+1)+(1ς)(+1)2|}

    and

    |a3|min{+ς+2(+2)(+1),1(+1)2+1+2}.

    Proof. Assume that fBΣ(;ϑ) and that f1=g. We consider the holomorphic functions Θ,Υ:UU, where Θ(0)=Υ(0)=0, satisfying the following criteria:

    z1f(z)(f(z))1=ϑ(Θ(z)),zU (3.1)

    and

    w1g(w)(g(w))1=ϑ(Υ(w)),wU. (3.2)

    Define the functions m and n by

    m(z)=1+Θ(z)1Θ(z)=1+m1z+m2z2+

    and

    n(z)=1+Υ(z)1Υ(z)=1+n1z+n2z2+.

    It follows that m, n are analytic functions in U, where m(0)=1=n(0). Then, we get Θ,Υ:UU, where m and n are functions with a positive real part in U.

    But, we have

    Θ(z)=1m(z)m(z)+1=12[m1z+(m2m212)z2]+,zU (3.3)

    and

    Υ(z)=1n(z)n(z)+1=12[n1z+(n2n212)z2]+,zU. (3.4)

    By substituting (3.3) and (3.4) into (3.1) and (3.2) and applying (2.1), we get

    z1f(z)(f(z))1=ϑ(Θ(z))=e(m(z)1m(z)+1+ς(m(z)1m(z)+1)22)=1+12m1z+[m22+(ς1)m218]z2+ (3.5)

    and

    w1g(w)(g(w))1=ϑ(Υ(w))=e(n(w)11+n(w)+ς(n(w)1n(w)+1)22)=1+12n1w+[n22+(ς1)n218]w2+ (3.6)

    Equating the coefficients in (3.5) and (3.6) yields

    (+1)a2=12m1, (3.7)
    (+2)a3+12(+2)(1)a22=m22+(ς1)m218, (3.8)
    (+1)a2=12n1 (3.9)

    and

    (+2)(2a22a3)+12(+2)(1)a22=n22+(ς1)n218. (3.10)

    From (3.7) and (3.9), we have

    m1=n1 (3.11)

    and

    2(+1)2a22=14(m21+n21). (3.12)

    If we add (3.8) to (3.10), we obtain

    (+2)(+1)a22=12(m2+n2)+18(ς1)(m21+n21). (3.13)

    Substituting from (3.12) the value of m21+n21 in the relation (3.13), we get

    a22=m2+n22[(+2)(+1)+(1ς)(+1)2]. (3.14)

    Applying Lemma 3.1 for the coefficients m1,m2,n1, and n2 in (3.12) and (3.14), we get

    |a2|1+1,|a2|2|(+2)(+1)+(1ς)(+1)2|.

    Applying (3.11) and subtracting (3.10) from (3.8) yields m21=n21, which is the bound on |a3|,

    2(+2)(a3a22)=12(m2n2). (3.15)

    Substituting a22 from (3.12) into (3.15) yields the following result:

    a3=m21+n218(+1)2+m2n24(+2).

    So, we have

    |a3|1(+1)2+1+2.

    Also, substituting the value of a22 from (3.13) into (3.15), we get

    a3=m2n24(+2)+m2+n22(+2)(+1)+(ς1)(m21+n21)8(+2)(+1)

    and we have

    |a3|+ς+2(+2)(+1).

    Theorem 3.2. LetfOΣ(ϰ;ϑ) (12ϰ1) and f be given by (1.1). Then,

    |a2|min{(2ϰ+1)216,2ϰ+12|2(ϰς)+3|}

    and

    |a3|min{(2ϰ+1)(3ς+5)24,2ϰ+112+(2ϰ+1)216}.

    Proof. Assume that fOΣ(ϰ;ϑ) and g=f1. Specifically, there exist holomorphic functions Θ,Υ:UU, hence

    2ϰ12ϰ+1+22ϰ+1(1+zf(z)f(z))=ϑ(Θ(z)),wherezU (3.16)

    and

    2ϰ12ϰ+1+22ϰ+1(1+wg(w)g(w))=ϑ(Υ(w)),wherewU, (3.17)

    where Θ(z) and Υ(z) have the forms (3.3) and (3.4). From (3.16), (3.17), and (2.1), we deduce that

    2ϰ12ϰ+1+22ϰ+1(1+zf(z)f(z))=ϑ(Θ(z))=e(m(z)1m(z)+1+ς(m(z)1m(z)+1)22)=1+12m1z+[m22+(ς1)m218]z2+ (3.18)

    and

    2ϰ12ϰ+1+22ϰ+1(1+wg(w)g(w))=ϑ(Υ(w))=e(n(w)1n(w)+1+ς(n(w)1n(w)+1)22)=1+12n1w+[n22+(ς1)n218]w2+ (3.19)

    Equating the coefficients in (3.18) and (3.19), yields

    42ϰ+1a2=12m1, (3.20)
    122ϰ+1a382ϰ+1a22=m22+(ς1)m218, (3.21)
    42ϰ+1a2=12n1 (3.22)

    and

    122ϰ+1(2a22a3)82ϰ+1a22=n22+(ς1)n218. (3.23)

    From (3.20) and (3.22), we have

    m1=n1 (3.24)

    and

    32(2ϰ+1)2a22=14(m21+n21). (3.25)

    If we add (3.21) to (3.23), we obtain

    82ϰ+1a22=12(m2+n2)+18(ς1)(m21+n21). (3.26)

    Substituting from (3.25) the value of m21+n21 in the relation (3.26), we deduce that

    a22=(2ϰ+1)2(m2+n2)16(2(ϰς)+3). (3.27)

    Applying Lemma 3.1 for the coefficients m1,m2,n1, and n2 in (3.25) and (3.27), we get

    |a2|(2ϰ+1)216,|a2|2ϰ+12|2(ϰς)+3|.

    Subtracting (3.23) from relation (3.21) and applying (3.24), we get |a3|.

    This yields m21=n21, hence

    242ϰ+1(a3a22)=12(m2n2), (3.28)

    then by substituting from (3.25) the value of a22 into (3.28), we get

    a3=(2ϰ+1)(m2n2)48+(2ϰ+1)2(m21+n21)128.

    So, we have

    |a3|2ϰ+112+(2ϰ+1)216.

    Also, substituting the value of a22 from (3.26) into (3.28), we get

    a3=(2ϰ+1)(m2n2)48+(2ϰ+1)(m2+n2)16+(2ϰ+1)(ς1)(m21+n21)64

    and we have

    |a3|(2ϰ+1)(3ς+5)24.

    Utilizing a22 and a3 values, and spurred by Zaprawa's recent work [53], we prove the Fekete-Szegö problem for fBΣ(;ϑ) and fOΣ(ϰ;ϑ) in the following theorems.

    Theorem 3.3. For a non-negative integer and R, let fBΣ(;ϑ) be of the form (1.1). Then,

    |a3a22|{1+2;|1||(+2)(+1)+(1ς)(+1)2|2(+2),2|1||(+2)(+1)+(1ς)(+1)2|;|1||(+2)(+1)+(1ς)(+1)2|2(+2).

    Proof. It follows from (3.14) and (3.15) that

    a3a22=m2n24(+2)+(1)a22=m2n24(+2)+(m2+n2)(1)2[(+2)(+1)+(1ς)(+1)2]=12[(ψ(,ς)+12(+2))m2+(ψ(,ς)12(+2))n2],

    where

    ψ(,ς)=1(+2)(+1)+(1ς)(+1)2.

    According to Lemma 3.1, we find that

    |a3a22|{1+2,0|ψ(,ς)|12(+2),2|ψ(,ς)|,|ψ(,ς)|12(+2).

    After some computations, we obtain

    |a3a22|{1+2;|1||(+2)(+1)+(1ς)(+1)2|2(+2),2|1||(+2)(+1)+(1ς)(+1)2|;|1||(+2)(+1)+(1ς)(+1)2|2(+2).

    Putting =1 in Theorem 3.3, we get the next result:

    Corollary 3.1. If fBΣ(;ϑ) is of the form (1.1), then we have that

    |a3a22|1+2.

    Theorem 3.4. For 12ϰ1 and R, let fOΣ(ϰ;ϑ) be of the form (1.1). Then,

    |a3a22|{16;|1||2ς|3,|1|2|2ς|;|1||2ς|3.

    Proof. It follows from (3.27) and (3.28) that

    a3a22=(2ϰ+1)(m2n2)48+(1)a22=(2ϰ+1)(m2n2)48+(2ϰ+1)2(m2+n2)(1)16(2(ϰς)+3)=116[(ϕ(,ς)+2ϰ+13)m2+(ϕ(,ς)2ϰ+13)n2],

    where

    ϕ(,ς)=(2ϰ+1)2(1)2(ϰς)+3.

    According to Lemma 3.1, we find that

    |a3a22|{2ϰ+112,0|ϕ(,ς)|2ϰ+13,14|ϕ(,ς)|,|ϕ(,ς)|2ϰ+13.

    After some computations, we obtain

    |a3a22|{2ϰ+112;|1|(2ϰ+1)|2(ϰς)+3|3(2ϰ+1)2,(2ϰ+1)2|1|4|2(ϰς)+3|;|1|(2ϰ+1)|2(ϰς)+3|3(2ϰ+1)2.

    Fixing =1 in Theorem 3.4, we get the following result:

    Corollary 3.2. If fOΣ(ϰ;ϑ) is of the form (1.1), then

    |a3a22|2ϰ+112.

    Remark 3.1. =0 and ϰ=12 give the results of Cotȋrlǎ and Wanas (see [15]).

    Motivated by many recent advances on the Fekete-Szegö functional and Taylor-Maclaurin coefficient estimations, we defined new families of holormorphic bi-univalent functions BΣ(;ϑ) and OΣ(ϰ;ϑ) associated with generalized telephone numbers are presented and thoroughly examined in this article. For functions in these families, we determined Taylor-Maclaurin coefficient inequalities and examined the well-known Fekete-Szegö issue. Furthermore, the generic coefficients |an|, n4, for the functions of these new classes remain unbounded. We also opted to utilize a significant finding from a recently released evaluate-cum-explanatory paper by Srivastava ([37], p. 340) to extend our study based on the q-difference operator. This observation pointed out that using some seemingly parametric and argumentative versions of the extra parameter p is redundant; the effects for the new or previously mentioned qanalogs could be easily (and possibly trivially) translated into corresponding effects for the so-called (p;q)analogues (with 0<|q|1). Further, one can obtain the second Hankel determinant inequalities for function classes studied in this article (see [42,43,44,45,46,47] and references cited therein).

    The authors declare that they have not used Artificial Intelligence tools in the creation of this article.

    The authors extend their appreciation to the Deanship of Scientific Research at King Khalid University for funding this work through a large group research project under grant number RGP2/432/44.

    The authors declare that they have no conflicts of interest.



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