Research article

Regions of variability for a subclass of analytic functions

  • Received: 31 December 2019 Accepted: 26 March 2020 Published: 31 March 2020
  • MSC : 30C45, 30C55, 30C80

  • Let AC, B[1,0) and α(π2,π2). Then Cα[A,B] denotes the class of analytic functions f in the open unit disc with \lt i \gt f \lt /i \gt (0) = 0 = \lt i \gt f \lt /i \gt '(0)-1 such that eiα(1+zf(z)f(z))=cosαp(z)+isinα, with p(z)=1+Aw(z)1+Bw(z), where w(0)=0 and |w(z)|<1. Region of variability problems provides accurate information about a class of univalent functions than classical growth distortion and rotation theorems. In this article we find the regions of variability Vλ(z0,A,B) for logf(z0) when f ranges over the class Cα[λ,A,B] defined as Cα[λ,A,B]={fCα[A,B]:f(0)=(AB)eiαcosα} for any fixed z0E and λ¯E. As a consequence, the regions of variability are also illustrated graphically for different sets of parameters.

    Citation: Mohsan Raza, Wasim Ul Haq, Jin-Lin Liu, Saddaf Noreen. Regions of variability for a subclass of analytic functions[J]. AIMS Mathematics, 2020, 5(4): 3365-3377. doi: 10.3934/math.2020217

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  • Let AC, B[1,0) and α(π2,π2). Then Cα[A,B] denotes the class of analytic functions f in the open unit disc with \lt i \gt f \lt /i \gt (0) = 0 = \lt i \gt f \lt /i \gt '(0)-1 such that eiα(1+zf(z)f(z))=cosαp(z)+isinα, with p(z)=1+Aw(z)1+Bw(z), where w(0)=0 and |w(z)|<1. Region of variability problems provides accurate information about a class of univalent functions than classical growth distortion and rotation theorems. In this article we find the regions of variability Vλ(z0,A,B) for logf(z0) when f ranges over the class Cα[λ,A,B] defined as Cα[λ,A,B]={fCα[A,B]:f(0)=(AB)eiαcosα} for any fixed z0E and λ¯E. As a consequence, the regions of variability are also illustrated graphically for different sets of parameters.


    Let A be the class of functions f analytic in the open unit disc E={z:|z|<1, zC} with the usual normalization f(0)=f(0)1=0 and S be the subclass of A consisting of functions which are univalent in E. Consider that A as a topological vector space endowed with the topology of uniform convergence over a compact subsets of E. Also let B denote the class of analytic functions w in E such that |w(z)|<1 and w(0)=0. A function f is said to be subordinate to a function  g written as fg, if there exists a Schwarz function wB such that f(z)=g(w(z)). In particular if g is univalent in E, then f(0)=g(0) and f(E)g(E).

    A set D in the complex plane is said to be starlike with respect to a point w0, an interior point of D if the line segment with initial point w0 lies entirely in D. If a function f maps E onto a domain that is starlike with respect to w0, then we say that f is starlike with respect to w0. In the special case that f is starlike function with respect to origin. The class of univalent starlike functions with respect to origin is denoted by S. The class of starlike functions with respect to the origin have been studied extensively, for some details [5,6].

    In 1933 Spacek [19] extended the idea of starlike functions by using the logarithmic spirals instead of line segment. Let α(π2,π2). The curve γα:texp(teiα), tR and its rotation eiθγα(t), θR are called α-spirals. A domain DC is said to be α-spirallike with respect to the origin if the spiral with initial point 0 to every point in D lies in D. A function fA is spirallike if it maps E onto a domain which is spirallike with respect to 0. The class of spirallike functions is denoted by Sα. In otherwise

    Sα={fA:Re(eiαzf(z)f(z))>0, zE}.

    Kim and Sugawa [10] introduced the notion of α-argument. Consider that θ=argαw with weiθγα(R). By using the α-argument, it is clear that fSα if and only if

    θ(argαf(reiθ))>0 (θR,0<r<1).

    For some details about the spirallike functions [1,5,6]. A function f with f(0)=f(0)1=0 is said to be Robertson functions if

    Re{eiα(1+zf(z)f(z))}>0, zE.

    The class of Robertson functions is denoted by Cα and defined by Robertson [17]. It is clear that C0=C, usual class of convex functions. In the view of above discussions about the spirallike functions and Robertson functions, we have the following relation. Let fA. Then fCα if and only if zfSα. By using the concept of Janowski [8], Sen et al. [18] studied the class Cα[A,B]. Let AC, B[1,0) and α(π2,π2). Then Cα[A,B] denotes the class of analytic functions f in the open unit disc with f(0)=0= f(0)1 such that

    eiα(1+zf(z)f(z))=cosαp(z)+isinα,

    with

    p(z)=1+Aw(z)1+Bw(z).

    The single-valued branch of logarithms for f(z) when fCα[A,B] is denoted by logf(z) with logf(0)=0. Yanagihara [21,22] determined the region of variability for the class of convex functions. Ponnusamy et al. [13] found the region of variability for some subclasses of univalent functions. For some work on region of variability, [7,11,12,13,14,15,16] and references therein.

    Using the Herglotz representation for Janowski functions, it can be seen that for fCα[A,B] there exists a unique positive unit measure μ in (π,π] such that

    1+zf(z)f(z)=eiα[cosαππ1+Azeit1+Bzeitdμ(t)+isinα]. (1.1)

    This shows that

    logf(z)=ABBeiαcosαππBeit1+Bzeitdμ(t). (1.2)

    It follows from (1.2) that for each fixed z0E, the region of variability is the set Vλ[z0,A,B] given as

    {ABBeiαcosαlog(1+Bz):|z||z0|}.

    Let

    pf(z)=eiα(1+zf(z)f(z)).

    Then there exists a Schwarz function wB, such that

    w(z)=pf(z)eiαAcosα+iBsinαBpf(z). (1.3)

    Let fCα[A,B]. Then by applying Schwarz lemma, that is |wp(0)|1 [4], we get

    |f(0)|=(AB)cosα|ωf(0)|(AB)cosα,

    for some λ¯E, Now for λ¯E={zC:|z|1} and z0E, we introduce

    Cα[λ,A,B]={fCα[A,B]:f(0)=λ(AB)eiαcosα}

    and

    Vλ(z0,A,B)={logf(z0):fCα[λ,A,B]}.

    The aim of this article is to investigate the region of variability Vλ(z0,A,B) for the class fCα[λ,A,B].

    We start our investigations by studying certain general properties of the set Vλ(z0,A,B) such as compactness and convexity.

    Proposition 2.1. (i) Vλ(z0,A,B) is a compact subset of C.

    (ii) Vλ(z0,A,B) is a convex subset of C.

    (iii) If |λ|=1 or z0=0, then Vλ(z0,A,B)={ABBeiαcosαlog(1+Bλz0)} and if |λ|<1 and z00, then the set Vλ(z0,A,B) has eiαcosαlog(1+Bλz0) an interior point.

    Proof. (ⅰ) Since Cα[λ,A,B] is a compact subset of C, therefore Vλ(z0,A,B) is also compact.

    (ⅱ) Let f1,f2Cα[λ,A,B]. Then for 0t1, the function

    f(z)=z0(f1(ς))1t(f2(ς))tdς

    is also in Cα[λ,A,B], therefore Vλ(z0,A,B) is convex because logf(z)=(1t)logf1(z)+tlogf2(z), t[0,1].

    (ⅲ)Since |λ|=|wf(0)|=1, then from Schwarz lemma, we obtain wf(z)=λz, which yields p(z)=1+λAz1+λBz. This implies that

    logf(z)=ABBeiαcosαlog(1+Bλz0).

    Therefore

    Vλ(z0,A,B)={ABBeiαcosαlog(1+Bλz0)}.

    This also trivially holds true when z0=0. For λE and α¯E, set

    δ(z,λ)=z+λ1+¯λz,
    Fa,λ(z)=z0(expς20eiαcosα(AB)δ(aς1,λ)1+Bς1δ(aς1,λ))dς1)dς2, zE. (2.1)

    Then Fa,λ(z) is in Cα[λ,A,B] and wf(z)=zδ(az,λ). For fixed λE and z0E{0} the function

    EalogFa,λ(z)=z00eiαcosα(AB)(aς+λ)1+(a¯λ+Bλ)ς+aBς2dς

    is a non-constant analytic function of aE, and therefore is an open mapping. Hence logF0,λ(z)={ABBeiαcosαlog(1+Bλz0)} is an interior point of {logFa,λ(z):aE}Vλ(z0,A,B).

    Keeping in view the above proposition, it is sufficient to find Vλ(z0,A,B) for 0λ<1 and z0E{0}.

    In this section, we state and prove some results which are needed in the proof of our main theorem.

    In the following proposition, we prove that for fCα[λ,A,B], the ratio f(z)/f(z) is contained in a closed disc with center q(z,λ) and radius r(z,λ).

    Proposition 3.1. For Cα[λ,A,B], we have

    |f(z)f(z)q(z,λ)|r(z,λ), (3.1)

    where

    q(z,λ)=D(z,λ)+|z|2|τ(z,λ)|2E(z,λ)1|z|2|τ(z,λ)|2,r(z,λ)=|z||τ(z,λ)||D(z,λ)+E(z,λ)|1|z|2|τ(z,λ)|2. (3.2)

    Proof. Since fCα[λ,A,B]. Then by using Schwarz lemma for wpB with wp(0)=λ such that

    |wf(z)zλ1¯λwf(z)z||z|. (3.3)

    Now from (1.3) this can be written equivalently as

    |f(z)f(z)D(z,λ)f(z)f(z)+E(z,λ)||z||τ(z,λ)|, (3.4)

    where

    D(z,λ)=λeiα(AB)cosα1+Bλz,  E(z,λ)=(BA)eiαcosα_λ+Bz,  τ(z,λ)=_λBz1+Bλz. (3.5)

    This is equivalent to

    |f(z)f(z)D(z,λ)+|z|2|τ(z,λ)|2E(z,λ)1|z|2|τ(z,λ)|2||z||τ(z,λ)||A(z,λ)+B(z,λ)|1|z|2|τ(z,λ)|2. (3.6)

    Now after simple calculations, we have

    1|z|2|τ(z,λ)|2=1B2|z|4+2B(1|z|2)Reλz+|λ|2|z|2(B21)|1+Bλz|2.

    Also

    D(z,λ)+E(z,λ)=eiαcosα(AB)(|λ|21)(1+Bλz)(_λ+Bz)

    and

    D(z,λ)+|z|2|τ(z,λ)|2E(z,λ)=eiα(AB)cosα{λ(1|z|2)+B_z(|λ|2|z|2)}|1+Bλz|2.

    By setting

    q(z,λ)=D(z,λ)+|z|2|τ(z,λ)|2E(z,λ)1|z|2|τ(z,λ)|2,r(z,λ)=|z||τ(z,λ)||D(z,λ)+E(z,λ)|1|z|2|τ(z,λ)|2.

    The relation (3.1) occurs from (3.6) and the above relations. Equality is attained in (3.1) when f=Feiθ,λ(z), for some zE. Conversely if equality occurs in (3.1) for some z E{0}, then equality must hold in (3.3). Thus by Schwarz lemma there exists θR such that wf(z)=zδ(eiθz,λ) for all zE. This implies f=Feiθ,λ.

    Geometrically the above proposition means that the functional logf lies in the closed disk centred at q(z,λ) with radius r(z,λ).

    For λ=0, we have the following special result which gives us bounds on pre-Schwarzian norm of locally univalent functions.

    Corollary 3.2. Let fCα[0,A,B]. Then

    |f(z)f(z)eiα(AB)cosα B_z|z|21B2|z|4||z||AB|cosα1B2|z|4.

    Therefore

    (1|B||z|2)|f(z)f(z)||AB||z|cosα.

    Since |B|1, so

    (1|z|2)|f(z)f(z)||AB||z|cosα.

    The pre-Schwarzian norm for locally univalent functions is defined as

    f=supzE(1|z|2)|f(z)f(z)|.

    It is well-known that f6, if f is univalent. Becker and Pommerenke [2] proved that if f1, then f is univalent in E and this bound is sharp. Yamashita [20] proved that if f is convex, then f1. The norm estimates for some subclasses of univalent functions are studied by many authors. For some details [3,9]. From Corollary 3.2, it is evident that for f(0) and A=1,B=1, we have f2cosα for Robertson functions. This result was proved by Ponnusamy et al. [15] also for α=0, we have f2.

    In the following result, we prove that the set Vλ(z0,A,B) is contained in a closed disc with centre Q(λ,r) and radius R(λ,r).

    Corollary 3.3. Consider the curve γ:z(t), 0t1 in E with z(0)=0 and z(1)=z0, then

    Vλ(z0,A,B)_E(Q(λ,r),R(λ,r))={ωC:|ωQ(λ,r)|R(λ,r)},

    with

    Q(λ,r)=10q(z(t),λ)z(t)dt,R(λ,r)=10r(z(t),λ)z(t)dt,

    where q(z,λ) and r(z,λ) are given in Proposition 3.1.

    Proof. Suppose that fCα[λ,A,B], then from proposition 3.1, we get

    |logf(z0)Q(λ,r)|=|10{f(z)f(z)q(z(t),λ)}z(t)dt|10|f(z)f(z)q(z(t),λ)||z(t)|dt.

    Now using proposition 3.1, we get

    |logf(z0)Q(λ,r)|10r(z(t),λ)|z(t)|dt=R(λ,r).

    This shows logf(z0) ¯D(Q(λ,r),R(λ,r)). Hence the required result.

    We need the following lemma which ensures the existence of normalized starlike function which is useful in the proof of next result.

    Lemma 3.4. For θR and |λ|<1, the function

    G(z)=z0eiθζ2(1+(¯λeiθ+Bλ)ζ+Beiθζ2)2dζ,  zE,

    has zeros of order 2 at the origin and no zero elsewhere in E. Moreover, there exists a starlike normalized univalent function G0 in E such that G=12eiθG20.

    The above lemma is due to Ponnusamy et al. [7]. In the below proposition we show that logFeiθ,λ(z0) lies on the boundary of the set Vλ(z0,A,B).

    Proposition 3.5. Let z0E{0}. Then for θ(π,π], we have logFeiθ,λ(z0)Vλ(z0,A,B). Further if logf(z0)=logFeiθ,λ(z0) for fCα[λ,A,B], then f=Feiθ,λ.

    Proof. Using 2.1, we have

    Fa,λ(z)=z0(expξ20eiαcos(AB)δ(aξ1,λ)1+Bξ1δ(aξ1,λ)dξ1)dξ2.

    Therefore

    Fa,λ(z)Fa,λ(z)=eiαcos(AB)δ(az,λ)1+Bzδ(az,λ)=eiα(AB)cosα (az+λ)1+(_λa+Bλ)z+Baz2.

    From (3.5), it follows that

    Fa,λ(z)Fa,λ(z)D(z,λ)=eiα(AB)cosα (1|λ|2)az{1+(_λa+Bλ)z+Baz2}(1+Bzλ)Fa,λ(z)Fa,λ(z)+E(z,λ)=eiα(AB)cosα (|λ|21){1+(_λa+Bλ)z+Baz2}(_λ+Bz).

    Therefore

    Fa,λ(z)Fa,λ(z)q(z,λ)=Fa,λ(z)Fa,λ(z)D(z,λ)+|z|2|τ(z,λ)|2E(z,λ)1|z|2|τ(z,λ)|2=11|z|2|τ(z,λ)|2{Fa,λ(z)Fa,λ(z)D(z,λ)|z|2|τ(z,λ)|2(Fa,λ(z)Fa,λ(z)+E(z,λ))}=eiα(AB)cosα(1|λ|2)¯(1+(¯λeiθ+Bλ)z+Beiθz2){1B2|z|4+2B(1|z|2)Reλz+|λ|2|z|2(B21)}{1+(_λa+Bλ)z+Baz2}.

    Putting a=eiθ, we get

    Feiθ,λ(z)Feiθ,λ(z)q(z,λ)=r(z,λ)eiθeiαz|z||1+(_λeiθ+Bλ)z+Beiθz2|2(1+(_λeiθ+Bλ)z+Beiθz2)2.

    By using Lemma 3.4, we obtain

    Feiθ,λ(z)Feiθ,λ(z)q(z,λ)=r(z,λ)eiαG(z)|G(z)|. (3.7)

    Using the argument of Lemma 3.4 that G=21eiθG20, where G0 is starlike in E with G0(0)=G0(0)1=0, for any z0E{0} the linear segment joining 0 and G0(z0) lies entirely in G0(E). Let γ0 be the curve defined by

    γ0:z(t)=G10(tG0(z0)), t[0,1].

    Since G(z(t))=21eiθ(G0(z(t)))2=21eiθ(tG0(z0))2=t2G(z0). Differentiation w.r.t t gives us

    G(z(t))z(t)=2tG(z0),  t[0,1]. (3.8)

    Therefore

    {Feiθ,λ(z)Feiθ,λ(z)q(z(t),λ)}z(t)=r(z(t),λ)eiαG(z0)|G(z0)||z(t)|.

    This relation together with (3.7), we get

    logFeiθ,λ(z)Q(γ0,λ)=10(Feiθ,λ(z)Feiθ,λ(z)q(z,λ))z(t)dt=10r(z(t),λ)eiαG(z(t))z(t)|G(z(t))z(t)||z(t)|dt=eiαG(z0)|G(z0)|10r(z(t),λ)|z(t)|dt=eiαG(z0)|G(z0)|R(λ,γ0). (3.9)

    This shows that logFeiθ,λ(z)E(Q(γ0,λ),R(γ0,r)), where Q(λ,γ0) and R(λ,γ0) are defined as in Corollary 3.3. Also we have logFeiθ,λ(z0)Vλ(z0,A,B), therefore logFeiθ,λ(z0)Vλ(z0,A,B).

    Now we have to prove logf(z0)=logF(z0) for some fCα[λ,A,B], we have

    h(t)=eiα|G(zo)|G(zo){f(z(t))f(z(t))q(z(t),λ)}z(t) (3.10)
    k(t)=eiα|G(zo)|G(zo){F(z(t))F(z(t))q(z(t),λ)}z(t),

    where γ0:z(t), 0t1. Then the function h is continuous and

    |h(t)|=|f(z(t))f(z(t))q(z(t),λ)||z(t)|.

    Using Proposition 3.1, we have

    |h(t)|r(z(t),λ)|z(t)|.

    Now using Proposition 3.1, we get |h(t)|r(z(t),λ)|z(t)|. Further from (3.9), we have From (3.7) and (3.8), this implies that f(z)f(z)=Feiθ,λ(z)Feiθ,λ(z) on γ0. The identity theorem for analytic functions yields us f=Feiθ,λ, zE.

    In our main result, we give precise description of regions of variability for the class Cα[λ,A,B] and show that the boundary Vλ(z0,A,B) is a Jordan curve.

    Theorem 3.6. Let λE and z0E{0}. Then boundary Vλ(z0,A,B) is the Jordan curve given by

    (π,π]θlogFeiθ,λ(z0)=z00eiαcosα(AB)δ(aς,λ)1+Bςδ(aς,λ))dς.

    If logf(z0)=logFeiθ,λ(z0) for some fCα[λ,A,B] and θ(π,π], then f(z)=Feiθ,λ(z).

    Proof. First we have to show that the curve

    (π,π]θlogFeiθ,λ(z0)

    is simple. Let us assume that

    logFeiθ1,λ(z0)=logFeiθ2,λ(z0)

    for some θ1,θ2(π,π] with θ1θ2. Then the use of Proposition 3.5 yield us that Feiθ1,λ(z0)=Feiθ2,λ(z0), which further gives the following relation

    τ(wFeiθ1,λ(z)z,λ)=τ(wFeiθ2,λ(z)z,λ).

    This implies that

    B(zeiθ1+λ)+¯λ(1+¯λeiθ1z)1+¯λeiθ1z+λB(zeiθ1+λ)=B(zeiθ2+λ)+¯λ(1+¯λeiθ2z)1+¯λeiθ2z+λB(zeiθ2+λ).

    After some simplification, we obtain zeiθ1=zeiθ2, which leads us to a contradiction. Hence the curve is simple. Since Vλ(z0,A,B) is compact convex subset of C and has non-empty interior, therefore the boundary Vλ(z0,A,B) is a simple closed curve. From Proposition 3.5 the curve Vλ(z0,A,B) contains the curve (π,π]θlogFeiθ,λ(z0). Since a simple closed curve cannot contain any simple closed curve other than itself. Thus Vλ(z0,A,B) is given by (π,π]θlogFeiθ,λ(z0).

    The following figures show us the geometric view of our main theorem with various choices of involved parameters.

    Authors are thankful to the editor and anonymous referees for their valuable comments and suggestions.

    The authors declare no conflicts of interest.



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