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Research article

On new subclasses of bi-starlike functions with bounded boundary rotation

  • Received: 14 February 2020 Accepted: 17 March 2020 Published: 30 March 2020
  • MSC : 30C45, 30C50

  • In this paper, we introduce two new classes BλΣ(m,μ) of λ-pseudo bi-starlike functions and LηΣ(m,β) to determine the bounds for |a2| and |a3|, where a2, a3 are the initial Taylor coefficients of fBλΣ(m,μ) and fLηΣ(m,β). Also, we attain the upper bounds of the Fekete-Szegö inequality by means of the results of |a2| and |a3|.

    Citation: Yumao Li, K. Vijaya, G. Murugusundaramoorthy, Huo Tang. On new subclasses of bi-starlike functions with bounded boundary rotation[J]. AIMS Mathematics, 2020, 5(4): 3346-3356. doi: 10.3934/math.2020215

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  • In this paper, we introduce two new classes BλΣ(m,μ) of λ-pseudo bi-starlike functions and LηΣ(m,β) to determine the bounds for |a2| and |a3|, where a2, a3 are the initial Taylor coefficients of fBλΣ(m,μ) and fLηΣ(m,β). Also, we attain the upper bounds of the Fekete-Szegö inequality by means of the results of |a2| and |a3|.


    Let A denote the class of functions of the form

    f(z)=z+k=2akzk (1.1)

    which are analytic in the open unit disk U={z:zCand|z|<1}. Further, denote by S the class of all functions in A which are univalent in U and normalized by the condition f(0)=0=f(0)1.

    One of the important and well examined subclasses of S is the class S(α) of starlike functions of order α,(0α<1), defined by the condition

    (zf(z)f(z))>α

    and the class K(α)S of convex functions of order α,(0α<1), is defined by the condition

    (1+zf(z)f(z))>α.

    The class Bλ(α) of λ-pseudo-starlike functions of order α,(0α<1) was introduced and investigated by Babalola [1]. A function f, fA is in the class Bλ(α) if it satisfies

    (z(f(z))λf(z))>α,(λ>1;zU).

    In [1] it was showed that all pseudo-starlike functions are Bazilevič functions of type (11/λ) and of order α1/λ and univalent in U.

    In [13] Padmanabhan and Parvatham defined the classes of functions Pm(β) as follows:

    Definition 1.1. [13] Let Pm(β), with m2 and 0β<1, denote the class of univalent analytic functions P, normalized with P(0)=1, and satisfying

    2π0|ReP(z)β1β|dθmπ,

    where z=reiθU.

    For β=0, we denote Pm:=Pm(0), hence the class Pm represents the class of functions p analytic in U, normalized with p(0)=1, and having the representation

    p(z)=2π01zeit1+zeitdμ(t),

    where μ is a real-valued function with bounded variation, which satisfies

    2π0dμ(t)=2πand2π0|dμ(t)|m,m2.

    Details referring the above integral representation could be found in [13,Lemma 1]. Remark that P:=P2 is the well-known class of Carathéodory functions, i.e. the normalized functions with positive real part in U.

    Lemma 1.1.([6,Lemma 2.1]) Let the function Φ(z)=1+n=1hnzn, zU, be such that ΦPm(β). Then,

    |hn|m(1β),n1.

    Supposing that the functions p,qPm(β), with

    p(z)=1+k=1pkzkandq(z)=1+k=1qkzk,

    from Lemma 1.1 it follows that

    |pk|m(1β), (1.2)
    |qk|m(1β),for allk1. (1.3)

    It is well known that every univalent function fS of the form (1.1), has an inverse f1(w) defined in (|w|<r0(f);r0(f)14), where

    g(w)=f1(w)=wa2w2+(2a22a3)w3(5a325a2a3+a4)w4+ (1.4)

    A function fS is said to be bi-univalent in U if there exists a function gS such that g(z) is an univalent extension of f1 to U. Let Σ denote the class of bi-univalent functions in U. The functions z1z, log(1z), 12log(1+z1z) are in the class Σ [14]. However, the familiar Koebe function is not bi-univalent. Lewin [8] investigated the class of bi-univalent functions Σ and obtained a bound |a2|1.51. Further Brannan and Clunie [3], Brannan and Taha [4] also worked on certain subclasses of the bi-univalent function class Σ and obtained estimates for their initial coefficients. Various classes of bi-univalent functions were introduced and studied in recent times, the study of bi-univalent functions gained momentum mainly due to the work of Srivastava et al.[14]. Motivated by this, many researchers [2,5,11,14,15,16,17,18,19,20] recently investigated several interesting subclasses of the class Σ and found non-sharp estimates on the first two Taylor-Maclaurin coefficients.

    Motivated by the aforementioned work on bi-univalent functions and recent works in [7,10], in this paper we define two new subclasses BλΣ(m,μ), λ-bi-pseudo-starlike functions and LηΣ(m,β) of Σ and determine the bounds for the initial Taylor-Maclaurin coefficients of |a2| and |a3| for fBλΣ(m,μ) and fLηΣ(m,β).

    Definition 1.2. Assume that fΣ, λ1 and (f(z))λ is analytic in U with (f(0))λ=1. Furthermore, assume that g(z) is an univalent extension of f1 to U, and (g(z))λ is analytic in U with (g(0))λ=1. Then f(z) is said to be in the class BλΣ(m,μ) of λ-bi-pseudo-starlike functions if the following conditions are satisfied:

    z(f(z))λ(1μ)z+μf(z)Pm(β)(zU) (1.5)

    and

    w(g(w))λ(1μ)w+μg(w)Pm(β)(wU), (1.6)

    where 0μ1.

    Remark 1.1. For λ=1, a function fΣ is in the class B1Σ(m,μ)MΣ(m,μ) if the following conditions are satisfied:

    zf(z)(1μ)z+μf(z)Pm(β)andwg(w)(1μ)w+μg(w)Pm(β), (1.7)

    where z,wU and the function g is described in (1.4).

    Remark 1.2. For λ=1;μ=1, a function fΣ is in the class B1Σ(m,1)SΣ(m) if the following conditions are satisfied:

    zf(z)f(z)Pm(β)andwg(w)g(w)Pm(β), (1.8)

    where z,wU and the function g is described in (1.4).

    Remark 1.3. For λ=2;μ=1, a function fΣ is in the class B2Σ(m,1)GΣ(m) if the following conditions are satisfied:

    f(z)zf(z)f(z)Pm(β)andg(w)wg(w)g(w)Pm(β), (1.9)

    where z,wU and the function g is described in (1.4).

    Remark 1.4. For μ=0, a function fΣ is in the class BλΣ(m,0)RλΣ(m) if the following conditions are satisfied:

    (f(z))λPm(β)and(g(w))λPm(β), (1.10)

    where z,wU and the function g is described in (1.4).

    Remark 1.5. For λ=1;μ=0, a function fΣ is in the class B1Σ(m,0)NΣ(m) if the following conditions are satisfied:

    f(z)Pm(β)andg(w)Pm(β), (1.11)

    where z,wU and the function g is described in (1.4).

    Theorem 2.1. Let f(z) given by (1.1) be in the class BλΣ(m,μ), then

    |a2|min{m(1β)2λμ;m(1β)2λ2+λ(12μ)μ(1μ)}, (2.1)
    |a3|min{m(1β)3λμ+m(1β)[2λ2+λ(12μ)μ(1μ)];m(1β)3λμ(1+m(1β)(2λ22λ(μ+1)+μ2)(2λμ)2);m(1β)3λμ(1+m(1β)(2λ2+(2λμ)(2μ))(2λμ)2)}, (2.2)

    and

    |a3δa22|m(1β)3λμ,

    where

    δ=2λ2+(2λμ)(2μ)3λμ.

    Proof. It is known that g has the form

    g(w)=wa2w2+(2a22a3)w3(5a325a2a3+a4)w4+.

    Since fBλΣ(m,μ), there exists two analytic functions

    p(z):=1+p1z+p2z2+ (2.3)

    and

    q(w):=1+q1w+q2w2+, (2.4)

    then

    z[f(z)]λ(1μ)z+μf(z)=p(z), (2.5)
    w[g(w)]λ(1μ)w+μg(w)=q(w). (2.6)

    On the other hand, we have

    z[f(z)]λ(1μ)z+μf(z)=1+(2λμ)a2z+[(2λ22λ(μ+1)+μ2)a22+(3λμ)a3]z2+, (2.7)
    w[g(w)]λ(1μ)w+μg(w)=1(2λμ)a2w+[(2λ2+(2λμ)(2μ))a22(3λμ)a3]w2+. (2.8)

    Using (2.3), (2.4), (2.7) and (2.8) and comparing the like coefficients of z and z2, we get

    (2λμ)a2=p1, (2.9)
    (2λ22λ(μ+1)+μ2)a22+(3λμ)a3=p2, (2.10)
    (2λμ)a2=q1, (2.11)
    (2λ2+(2λμ)(2μ))a22(3λμ)a3=q2. (2.12)

    From (2.9) and (2.11), we find that

    a2=p12λμ=q12λμ; (2.13)

    from Lemma 1.1 it follows that

    |a2|m(1β)2λμ. (2.14)

    Adding (2.10) and (2.12), we have

    [4λ2+2λ(12μ)2μ(1μ)]a22=p2+q2, (2.15)
    a22=p2+q24λ2+2λ(12μ)2μ(1μ).

    Hence by Lemma 1.1

    |a2|22m(1β)2[2λ2+λ(12μ)μ(1μ)],
    |a2|m(1β)2λ2+λ(12μ)μ(1μ). (2.16)

    Subtracting (2.10) from (2.12), we obtain

    a3=(p2q2)2(3λμ)+a22,|a3|m(1β)3λμ+|a2|2=m(1β)3λμ+m(1β)[2λ2+λ(12μ)μ(1μ)].

    By using (2.9) and (2.10) and by simple computation, we get

    |a3|m(1β)3λμ(1+m(1β)(2λ22λ(μ+1)+μ2)(2λμ)2). (2.17)

    Again by using (2.9) and (2.12)

    |a3|m(1β)3λμ(1+m(1β)(2λ2+(2λμ)(2μ))(2λμ)2). (2.18)

    From (2.12) we have

    (2λ2+(2λμ)(2μ))3λμa22a3=q23λμ.

    Furthermore by

    |a3δa22|=|q2|3λμm(1β)3λμ,

    where

    δ=2λ2+(2λμ)(2μ)3λμ.

    This completes the proof of Theorem 2.1.

    Remark 2.1. Specializing λ,μ suitably as mentioned in Remarks 1.1 to 1.5 we can state the initial Taylor coefficients |a2|,|a3| and the inequality |a3δa22| for the function classes defined in Remarks 1.1 to 1.5.

    In [12], Obradovic et al. gave some criteria for univalence expressing by (f(z))>0, for the linear combinations

    η(1+zf(z)f(z))+(1η)1f(z),(η1,zU).

    Based on the above definition recently, in [9], Lashin introduced and studied the new subclass of bi-univalent functions. We define the following new bi-univalent function class:

    Definition 3.1. A function f(z)Σ given by (1.1) is said to be in the class LηΣ(m,β) if it satisfies the following conditions :

    η(1+zf(z)f(z))+(1η)1f(z)Pm(β) (3.1)

    and

    η(1+wg(z)g(w))+(1η)1g(w)Pm(β), (3.2)

    where η1,z,wU and the function g is given by (1.4).

    Theorem 3.1. Let f(z) be given by (1.1) be in the class LηΣ(m,β), η1. Then

    |a2|min{m(1β)2(2η1);m(1β)η+1}, (3.3)
    |a3|min{m(1β)3(3η1)+m(1β)1+η;m(1β)3(3η1)(1m(1β)2η1);m(1β)3(3η1)(1+m(1β)(5η1)2(12η)2)}, (3.4)

    and

    |a3ρa22|=|q2|3(3η1)m(1β)3(3η1),

    where

    ρ=2(5η1)3(3η1).

    Proof. It follows from (3.1) and (3.2) that

    η(1+zf(z)f(z))+(1η)1f(z)Pm(β) (3.5)

    and

    η(1+wg(z)g(w))+(1η)1g(w)Pm(β). (3.6)

    From (3.5) and (3.6), we have

    1+2(2η1)a2z+[3(3η1)a34(2η1)a22]z2+=1+p1z+p2z2+

    and

    12(2η1)a2w+[(10η2)a223(3η1)a3]w2=1+q1w+q2w2+.

    Now, equating the coefficients, we get

    (2η1)a2=p1, (3.7)
    3(3η1)a3+4(12η)a22=p2, (3.8)
    2(2η1)a2=q1 (3.9)

    and

    (10η2)a223(3η1)a3=q2. (3.10)

    From (3.7) and (3.9), we get

    a2=p12(2η1)=q12(2η1); (3.11)

    it follows that

    |a2|m(1β)2(2η1). (3.12)

    Now by adding (3.8) and (3.10), we obtain

    2(η+1)a22=p2+q2, (3.13)
    a22=p2+q22(η+1),

    which, by virtue of Lemma 1.1, implies that

    |a2|2m(1β)η+1.

    Hence

    |a2|m(1β)η+1. (3.14)

    Subtracting (3.10) from (3.8), we obtain

    a3=(p2q2)6(3η1)+a22,|a3|m(1β)3(3η1)+|a2|2=m(1β)3(3η1)+m(1β)1+η.

    By using (3.7) and (3.8) and by simple computation, we get

    |a3|m(1β)3(3η1)(1m(1β)2η1). (3.15)

    Again by using (3.7) in (3.10)

    |a3|m(1β)3(3η1)(1+m(1β)(5η1)2(12η)2). (3.16)

    From (3.10) we have

    2(5η1)3(3η1)a22a3=q23(3η1).

    Furthermore by

    |a3ρa22|=|q2|3(3η1)m(1β)3(3η1),

    where

    ρ=2(5η1)3(3η1).

    This completes the proof of Theorem 3.1.

    Corollary 3.2. Let f(z) be given by (1.1) be in the class LηΣ(m,β), η=1. Then

    |a2|min{m(1β)2;m(1β)2},
    |a3|min{3m(1β)2;m(1β)6(1m(1β));m(1β)6(1+2m(1β))}

    and

    |a3ρa22|=|q2|6m(1β)6,

    where

    ρ=43.

    In this paper, we introduce two new classes BλΣ(m,μ) of λ-pseudo bi-starlike functions and LηΣ(m,β) and obtain the estimates of |a2|, |a3| and the upper bounds of the Fekete-Szegö inequality, where a2 and a3 belong to fBλΣ(m,μ) and fLηΣ(m,β), respectively. In addition, we observe that, if we choose some suitable parameters λ, μ, η and m in the results involved, we can get some corresponding bounds.

    This work was supported by the Natural Science Foundation of the People's Republic of China (Grant No. 11561001), the Program for Young Talents of Science and Technology in Universities of Inner Mongolia Autonomous Region (Grant No. NJYT-18-A14), the Natural Science Foundation of Inner Mongolia of the People's Republic of China (Grant No. 2018MS01026), the Higher School Science Research Foundation of Inner Mongolia of the People's Republic of China (Grant No. NJZY18217) and the Natural Science Foundation of Chifeng of Inner Mongolia. Also, the authors would like to thank the referees for their valuable comments and suggestions, which was essential to improve the quality of this paper.

    The authors declare no conflicts of interest.



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    11. Ibtisam Aldawish, Prathviraj Sharma, Sheza M. El-Deeb, Mariam R. Almutiri, Srikandan Sivasubramanian, Initial Coefficient Bounds for Certain New Subclasses of Bi-Univalent Functions Involving Mittag–Leffler Function with Bounded Boundary Rotation, 2024, 16, 2073-8994, 971, 10.3390/sym16080971
    12. Anandan Murugan, Sheza M. El-Deeb, Mariam Redn Almutiri, Prathviraj Sharma, Srikandan Sivasubramanian, Certain new subclasses of bi-univalent function associated with bounded boundary rotation involving sǎlǎgean derivative, 2024, 9, 2473-6988, 27577, 10.3934/math.20241339
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    14. Anandan Murugan, Srikandan Sivasubramanian, Prathviraj Sharma, Gangadharan Murugusundaramoorthy, Faber Polynomial Coefficient Estimates of m-Fold Symmetric Bi-Univalent Functions with Bounded Boundary Rotation, 2024, 12, 2227-7390, 3963, 10.3390/math12243963
    15. Prathviraj Sharma, Srikandan Sivasubramanian, Gangadharan Murugusundaramoorthy, Nak Eun Cho, On a New Class of Concave Bi-Univalent Functions Associated with Bounded Boundary Rotation, 2025, 13, 2227-7390, 370, 10.3390/math13030370
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