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Research article

The Fekete-Szegö type inequalities for certain subclasses analytic functions associated with petal shaped region

  • Received: 05 December 2020 Accepted: 17 March 2021 Published: 01 April 2021
  • MSC : 30C45, 30C50

  • In the article we introduce several new subclasses of analytic functions associated with pedal shaped functions. By using differential subordination and convolution operator theory, we obtain the bound estimations of the coefficients a2 and a3, and the logarithmic coefficients d1 and d2 as well as Fekete-Szegö type functional inequalities for these subclasses.

    Citation: Pinhong Long, Xing Li, Gangadharan Murugusundaramoorthy, Wenshuai Wang. The Fekete-Szegö type inequalities for certain subclasses analytic functions associated with petal shaped region[J]. AIMS Mathematics, 2021, 6(6): 6087-6106. doi: 10.3934/math.2021357

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  • In the article we introduce several new subclasses of analytic functions associated with pedal shaped functions. By using differential subordination and convolution operator theory, we obtain the bound estimations of the coefficients a2 and a3, and the logarithmic coefficients d1 and d2 as well as Fekete-Szegö type functional inequalities for these subclasses.



    Let A denote the class of functions of the form

    f(z)=z+a2z2+a3z3+a4z4+, (1.1)

    which are analytic in the open unit disk D={z:∣z∣<1} and normalized by f(0)=0 and f(0)=1. Recall that, SA is the univalent function in D={z:∣z∣<1} and has the star-like and convex function classes as its sub-classes which their geometric conditions satisfy

    (zf(z)f(z))>0and(1+zf(z)f(z))>0, (1.2)

    respectively. The two well-known sub-classes have been used to define different subclasses of analytical functions in different direction with different perspective and their results are too voluminous in literature.

    For two functions f and g, f is said to be subordinate to g, written as fg, if there exists a Schwartz function w(z) such that

    f(z)=g(w(z)),zD, (1.3)

    where w(0)=0 and w(z)∣<1 for zD.

    Goodman [2] proposed the concept of conic domain to generalize convex function which generated the first parabolic region as an image domain of analytic function. Besides, he also introduced and studied the class UCV of uniformly convex functions which satisfy

    {1+(zψ)f(z)f(z)}>0,(z,ψD).

    Lately, Ma and Minda [8] and Rønning[15] independently studied the underneath characterization

    {1+zf(z)f(z)}>|zf(z)f(z)|,zD. (1.4)

    Rønning [15] also defined a class ST as below

    {zf(z)f(z)}>|zf(z)f(z)1|,zD. (1.5)

    Further, we say that f of the form (1.1) is in USD, if

    {f(z)}|f(z)1|,zD. (1.6)

    The above characterization given in (1.4), resulted in the first parabolic region of the form

    Ω={w;(w)>∣w1}, (1.7)

    which was later generalized by Kanas and Wisniowska [3,4] to

    Ωk={w;(w)>kw1},k0. (1.8)

    We note that Ωk represents the right half plane for k=0, hyperbolic region for 0<k<1, parabolic region for k=1 and elliptic region for k>1.

    From then on, the generalized conic region (1.8) has been studied by many researchers (see [10,12] and also references cited therein). Moreover, the conic domain Ω was generalized to domain Ω[A,B], 1B<A1, by Noor and Malik [13] via

    Ω[A,B]={u+iv:[(B21)(u2+v2)2(AB1)u+(A21)]2>[2(B+1)(u2+v2)+2(A+B+2)u2(A+1)]2+4(AB)2v2},

    which is called petal shaped region (also see [11]).

    A function p(z)UP[A,B], if and only if

    p(z)(A+1)˜p(z)(A1)(B+1)˜p(z)(B1), (1.9)

    where "" denotes subordination, and ˜p=1+2π2(log1+z1z)2.

    Fixing A=1 and B=1 in (1.9), the usual classes of functions studied by Goodman [1] and Kanas [3,4] can be obtained.

    Furthermore, the classes UCV[A,B] and ST[A,B] are uniformly Janowski convex and starlike defined below:

    A function fA is said to be in the class UCV[A,B] 1B<A1, if and only if

    ((B1)(1+zf(z)f(z))(A1)(B+1)(1+zf(z)f(z))(A+1))>|(B1)(1+zf(z)f(z))(A1)(B+1)(1+zf(z)f(z))(A+1)1|, (1.10)

    or equivalently

    1+zf(z)f(z)UP[A,B].

    A function fA is said to be in the class ST[A,B], 1B<A1, if and only if

    ((B1)zf(z)f(z)(A1)(B+1)zf(z)f(z)(A+1))>|(B1)zf(z)f(z)(A1)(B+1)zf(z)f(z)(A+1)1|, (1.11)

    or equivalently

    zf(z)f(z)UP[A,B].

    A function fA is said to be in the class USD[A,B], 1B<A1, if and only if

    ((B1)f(z)(A1)(B+1)f(z)(A+1))>|(B1)f(z)(A1)(B+1)f(z)(A+1)1|, (1.12)

    or equivalently

    f(z)UP[A,B].

    It can easily be seen that f(z)UCV[A,B]zf(z)ST[A,B]. Setting A=1 and B=1 in (1.10) and (1.11), we obtained the classes of functions investigated by Goodman [2] and Rønning [15].

    The relevant connection to Fekete-Szegö problem is a way of maximizing the non-linear functional |a3μa22| for various subclasses of univalent functions. To know much more of history, we refer the readers to [5,7,16]. Inspired by earlier work in [14], in this paper we study the coefficient inequalities for certain subclasses of analytical functions related to petal type region. The first few coefficient bounds and the relevant connection to Fekete-Szegö inequalities were obtained for the classes of functions defined. Also note that, the results obtained here have not been in literature and the varying of parameters involved can give rise to new or known results. For the purpose of the main results, the following lemmas and definitions are needed.

    Lemma 1.1. [1] Let P be the class of all analytic functions h(z) of the following form

    h(z)=1+n=1cnzn,(zD) (1.13)

    satisfying [h(z)]>0 and h(0)=1. Then cn∣≤2(nN) and the result is best possible for h(z)=1+ρz1ρz,|ρ|=1.

    The next lemmas give us a majorant for the coefficients of the functions of the class P, and more details may be found in [9]:

    Lemma 1.2. [9] If h(z)P is given by (1.13), then, for any complex μ,

    |c2μc21|2max{1,|2μ1|}

    and the result is sharp for the functions

    h0(z)=1+z1zorh(z)=1+z21z2,(zD).

    Lemma 1.3. [9] (Lemma 1 and Remark, pp. 162-163) Let h(z)P be given by (1.13). Then

    c2μc21∣≤{4μ+2,ifμ0,2,if0μ1,4μ2,ifμ1.

    When μ<0 or μ>1, the equality holds if and only if h1=1+z1z or one of its rotations. If 0<μ<1, then equality holds if and only if h2=1+z21z2 or one of its rotations. If μ=0, the equality holds if and only if

    h3(z)=(12+η2)1+z1z+(12η2)1z1+z,(0η1)

    or one of its rotations. If μ=1, then the sharp result holds for the following function

    1h3(z)=(12+η2)1+z1z+(12η2)1z1+z,(0η1)

    or one of its rotations. Although the above upper bound is sharp, when 0<μ<1, it can be improved as follows:

    |c2μc21|+μ|c1|22,(0<μ12) (1.14)

    and

    |c2μc21|+(1μ)|c1|22,(12<μ<1). (1.15)

    Definition 1.4. For 0λ1, and 1B<A1, a function fA is said to be in the class N[λ,A,B], if and only if

    ((B1)F(z)(A1)(B+1)F(z)(A+1))>|(B1)F(z)(A1)(B+1)F(z)(A+1)1|, (1.16)

    or equivalently (f(z))λ(zf(z)f(z))1λ=F(z)UP[A,B].

    Remark 1.5. We note that by fixing λ=0, then N[λ,A,B]ST[A,B] and λ=1, then N[λ,A,B]USD[A,B]

    Definition 1.6. For 0λ1, and 1B<A1, a function fA is said to be in the class M[λ,A,B], if and only if

    ((B1)G(z)(A1)(B+1)G(z)(A+1))>|(B1)G(z)(A1)(B+1)G(z)(A+1)1|, (1.17)

    or equivalently (f(z))λ(1+zf(z)f(z))1λ=G(z)UP[A,B].

    Remark 1.7. We note that by taking λ=0, then M[λ,A,B]UCV[A,B] and λ=1, then M[λ,A,B]USD[A,B]

    Definition 1.8. For 0λ1, and 1B<A1, a function fA is said to be in the class W[λ,A,B], if and only if

    ((B1)Q(z)(A1)(B+1)Q(z)(A+1))>|(B1)Q(z)(A1)(B+1)Q(z)(A+1)1|, (1.18)

    or equivalently (zf(z)f(z))λ(1+zf(z)f(z))1λ=Q(z)UP[A,B].

    Remark 1.9. Assuming λ=0, we note that W[λ,A,B]UCV[A,B] and λ=1, then W[λ,A,B]ST[A,B]

    In this section, we let 1B<A1, 0λ1, unless otherwise stated. To prove our main results we recall the following:

    Let hP of the form (1.13). Consider

    h(z)=1+w(z)1w(z),

    where w(z) is such that w(0)=0 and |w(z)|<1. Then, it follows easily that

    w(z)=h(z)1h(z)+1=c12z+(c22c214)z2+(c32c2c12+c318)z3+. (2.1)

    Now, if ˜p(z)=1+R1z+R2z2+, where R1=8π2,R2=163π2 and R3=18445π2 (see [6]), then we have

    ˜p(w(z))=1+R1w(z)+R2(w(z))2+R3(w(z))3+. (2.2)

    Hence, from (2.1) and (2.2) we get

    ˜p(w(z))=1+4c1π2z+4π2(c2c216)z2+4π2(c3c1c23+2c3145)z3+. (2.3)

    If pUP[A,B], from the relation (2.3), we may derive

    p(z)=(A+1)˜p(w(z))(A1)(B+1)˜p(w(z))(B1)=2+(A+1)4π2c1z+(A+1)4π2(c2c216)z2+2+(B+1)4π2c1z+(B+1)4π2(c2c216)z2+.

    Thereby, it implies that

    p(z)=1+2(AB)c1π2z+2(AB)π2(c2c2162(B+1)c21π2)z2+8(AB)π2×[((B+1)2π4+B+16π2+190)c31(B+1π2+112)c1c2+c34]z3+. (2.4)

    Theorem 2.1. Let fN[λ,A,B] and f be of the form (1.1). Then, we have

    |a2|4(AB)(1+λ)π2, (2.5)
    |a3|4(AB)(2+λ)π2max{1,2|˜Θ|} (2.6)

    for

    ˜Θ=2(B+1)π2(2+λ)(1λ)(AB)(1+λ)2π213.

    Furthermore, for a complex number μ, we get

    |a3μa22|4(AB)(2+λ)π2max{1,2|˜Λ|}, (2.7)

    where

    ˜Λ=2(B+1)π2(2+λ)(1λ2μ)(AB)(1+λ)2π213.

    Proof. Assume that fN[λ,A,B]. Then, it follows from the relation (1.9) and Definition 1.4 that

    (f(z))λ(zf(z)f(z))1λ=(A+1)˜p(w(z))(A1)(B+1)˜p(w(z))(B1),

    where w(z) is such that w(0)=0 and w(z)∣<1. From (2.4) we get

    (A+1)˜p(w(z))(A1)(B+1)˜p(w(z))(B1)=1+2(AB)c1π2z+2(AB)π2(c2c2162(B+1)c21π2)z2
    +8(AB)π2[((B+1)2π4+B+16π2+190)c31(B+1π2+112)c1c2+c34]z3+. (2.8)

    If f(z) is given by (1.1), then we have

    (f(z))λ(zf(z)f(z))1λ=1+(1+λ)a2z+12(2+λ)[2a3(1λ)a22]z2+. (2.9)

    From the comparison of coefficients of z and z2 in (2.8) and (2.9), we obtain

    a2=2(AB)c1π2(1+λ) (2.10)

    and

    12(2+λ)[2a3(1λ)a22]=2(AB)π2(c2c2162(B+1)c21π2). (2.11)

    By using (2.10) in (2.11), we get

    a3=2(AB)(2+λ)π2[c216c212(B+1)π2c21+(2+λ)(1λ)(AB)(1+λ)2π2c21]=2(AB)(2+λ)π2(c2ϑc21), (2.12)

    where

    ϑ=16+2(B+1)π2(2+λ)(1λ)(AB)(1+λ)2π2.

    In view of Lemma 1.1, from (2.10) we get

    |a2|4(AB)(1+λ)π2,

    and by applying Lemma 1.2 to (2.12), we get

    |a3|4(AB)(2+λ)π2max{1,|2ϑ1|}=4(AB)(2+λ)π2max{1,2|2(B+1)π2(2+λ)(1λ)(AB)(1+λ)2π213|}

    so that we get the desired result in (2.5) and (2.6).

    Now, for μC, we note that

    |a3μa22|=2(AB)(2+λ)π2|c2c21(16+2(B+1)π2(2+λ)(1λ2μ)(AB)(1+λ)2π2)|=2(AB)(2+λ)π2|c2c21|,

    where

    =16+2(B+1)π2(2+λ)(1λ2μ)(AB)(1+λ)2π2.

    By Lemma 1.2, we get

    |a3μa22|4(AB)(2+λ)π2max{1,2|2(B+1)π2(2+λ)(1λ2μ)(AB)(1+λ)2π213|},

    which yields the desired result in (2.7).

    Theorem 2.2. Let fM[λ,A,B] be of the form (1.1). Then

    |a2|2(AB)π2, (2.13)
    |a3|4(AB)3(2λ)π2max{1,2|˜Ξ|} (2.14)

    for

    ˜Ξ=2(B+1)π22(AB)(1λ)π213.

    Further, for a complex number μ, we have

    |a3μa22|4(AB)3(2λ)π2max{1,2|˜Π|} (2.15)

    for

    ˜Π=2(B+1)π2(AB)2π2[4(1λ)3μ(2λ)]13.

    Proof. Suppose that fM[λ,A,B] and of the form (1.1). Then, it follows from the relation (1.9) and Definition 1.6 that

    (f(z))λ(1+zf(z)f(z))1λ=(A+1)˜p(w(z))(A1)(B+1)˜p(w(z))(B1),

    where w(z) is such that w(0)=0 and w(z)∣<1. From (2.4) we assert that

    (A+1)˜p(w(z))(A1)(B+1)˜p(w(z))(B1)=1+2(AB)c1π2z+2(AB)π2(c2c2162(B+1)π2c21)z2+8(AB)π2×[((B+1)2π4+B+16π2+190)c31(B+1π2+112)c1c2+c34]z3+. (2.16)

    Since f is given by (1.1), we know

    (f(z))λ(1+zf(z)f(z))1λ=1+2a2z+[3(2λ)a34(1λ)a22]z2+. (2.17)

    By the comparison of coefficients of z and z2 in (2.16) and (2.17), we get

    a2=(AB)c1π2 (2.18)

    of which by Lemma 1.1 gives

    |a2|2(AB)π2,

    and

    a3=2(AB)3(2λ)π2[c2(16+2(B+1)π22(AB)(1λ)π2)c21]=2(AB)3(2λ)π2(c2ϑc21), (2.19)

    where

    ϑ=16+2(B+1)π22(AB)(1λ)π2.

    By Lemma 1.2, we can deduce that

    |a3|4(AB)3(2λ)π2max{1,|2ϑ1|}=4(AB)3(2λ)π2max{1,2|2(B+1)π22(AB)(1λ)π213|},

    which yields the desired result in (2.14).

    Now, for a complex number μ,

    |a3μa22|=2(AB)3(2λ)π2|c2c21(16+2(B+1)π22(1λ)(AB)π2+3μ(AB)(2λ)2π2)|=2(AB)3(2λ)π2|c2ϱc21|,

    where

    ϱ=16+2(B+1)π2(AB)2π2[4(1λ)3μ(2λ)].

    Hence, by means of Lemma 1.2 we get the desired result (2.15).

    Theorem 2.3. If the function fW[λ,A,B] is of the form (1.1), then

    |a2|4(AB)(2λ)π2, (2.20)
    |a3|2(AB)(32λ)π2max{1,2|˜Φ|} (2.21)

    for

    ˜Φ=2(B+1)π2+(AB)(λ2+5λ8)(2λ)2π213.

    Moreover, for a complex number μ, we obtain

    |a3μa22|2(AB)(32λ)π2max{1,2|˜Ψ|} (2.22)

    for

    ˜Ψ=2(B+1)π2+(AB)[λ2+5λ8+4(32λ)μ](2λ)2π213.

    Proof. Let fW[λ,A,B]. Then, applying the relation (1.9) and Definition 1.8 we have

    (zf(z)f(z))λ(1+zf(z)f(z))1λ=(A+1)˜p(w(z))(A1)(B+1)˜p(w(z))(B1), (2.23)

    where w(z) is such that w(0)=0 and |w(z)|<1. From (2.4) we get

    (A+1)˜p(w(z))(A1)(B+1)˜p(w(z))(B1)=1+2(AB)c1π2z+2(AB)π2(c2c2162(B+1)c21π2)z2+. (2.24)

    In view of (1.1), we obtain

    (zf(z)f(z))λ(1+zf(z)f(z))1λ=1+(2λ)a2z+[2(32λ)a3+12(λ2+5λ8)a22]z2+. (2.25)

    By the comparison of coefficients of z and z2 in (2.24) and (2.25), we get

    a2=2(AB)c1(2λ)π2 (2.26)

    and

    2(32λ)a3+12(λ2+5λ8)a22=2(AB)π2(c2c2162(B+1)π2c21).

    Then, by (2.26),

    a3=12(32λ)[2(AB)π2(c2c2162(B+1)π2c21)2(AB)2[λ2+5λ8](2λ)2π4c21]=(AB)(32λ)π2[c2c21(16+2(B+1)π2+(AB)(λ2+5λ8)(2λ)2π2)]. (2.27)

    Following the procedure as in the above theorems, we can get the desired results given by (2.20) and (2.21).

    Now, for a complex number μ,

    |a3μa22|=|(AB)(32λ)π2[c2c21(16+2(B+1)π2+(AB)[λ2+5λ8+4μ(32λ)](2λ)2π2)]|=(AB)(32λ)π2|c2ξc21|,

    where

    ξ=16+2(B+1)π2+(AB)[λ2+5λ8+4μ(32λ)](2λ)2π2.

    Therefore, in light of Lemmas 1.1 and 1.2 we get the desired result (2.22).

    If we choose real μ, then by Lemma 1.3 we derive the next results for Fekete-Szegö problem for these classes above.

    Theorem 2.4. If the function fN[λ,A,B] be of the form (1.1), and μR then

    |a3μa22|{8(AB)(2+λ)π2{2(B+1)π2+(2+λ)(1λ2μ)(AB)(1+λ)2π2+13},(μΥ1);4(AB)(2+λ)π2,(Υ1μΥ2);8(AB)(2+λ)π2{2(B+1)π2(2+λ)(1λ2μ)(AB)(1+λ)2π213},(μΥ2),

    where

    Υ1=1λ2[π26+2(B+1)](1+λ)22(2+λ)(AB)

    and

    Υ2=1λ2[5π26+2(B+1)](1+λ)22(2+λ)(AB).

    Moreover, we set

    Υ3=1λ2[π23+2(B+1)](1+λ)22(2+λ)(AB).

    Then, each of the following results holds:

    (A) For μ[Υ1,Υ3],

    |a3μa22|+(1+λ)2π2(˜Λ+12)2(2+λ)(AB)|a2|24(AB)(2+λ)π2;

    (B) For μ[Υ3,Υ2],

    |a3μa22|+(1+λ)2π2(˜Λ+12)2(2+λ)(AB)|a2|24(AB)(2+λ)π2,

    where

    ˜Λ=2(B+1)π2(2+λ)(1λ2μ)(AB)(1+λ)2π213.

    Proof. If fN[λ,A,B] is given by (1.1), based on the proof of Theorem 2.1 we see

    a3μa22=2(AB)(2+λ)π2[c2c21], (2.28)

    where

    =16+2(B+1)π2(2+λ)(1λ2μ)(AB)(1+λ)2π2.

    For R, we know that 1 is equivalent to μΥ2, and 0 is equivalent to μΥ1. Therefore, taking the modulus on both sides of the above equality, with the aid of the inequality in Lemma 1.3 we obtain the first estimates of Theorem 2.4.

    For the proof of the second part, note that 0<1/2 is equivalent to Υ1<μΥ3. By using the relations (2.28) and (2.10), and then by applying the inequality (1.14) of Lemma 1.3, we get

    2(AB)(2+λ)π2[|c2c21|+|c21|]=|a3μa22|+2(AB)(2+λ)π2|c21|=|a3μa22|+(1+λ)2π2(˜Λ+12)2(2+λ)(AB)|a22|4(AB)(2+λ)π2

    such that the required inequality (A) holds.

    Similarly, we can easily check that 1/2<1 is equivalent to Υ3μ<Υ2. From the relations (2.28) and (2.10), and the inequality (1.15) of Lemma 1.3 we obtain

    2(AB)(2+λ)π2[|c2c21|+(1)|c21|]=|a3μa22|+2(AB)(1)(2+λ)π2|c21|=|a3μa22|+(1+λ)2π2(˜Λ+12)2(2+λ)(AB)|a22|4(AB)(2+λ)π2,

    which is exactly the inequality (B).

    To show that the bounds are sharp, we define the functions Kpn (n=2,3,) with Kpn(0)=0=[Kpn](0)1, by

    (Kpn(z))λ(zKpn(z)Kpn(z))1λ=p(zn1)=2+2(A+1)π2(log1+zn11zn1)22+2(B+1)π2(log1+zn11zn1)2,

    where p(z) is as given in (1.9). Also, define the functions Fη and Gη, 0η1, respectively, with Fη(0)=0=Fη(0)1 and Gη(0)=0=Gη(0)1 by

    (Fη(z))λ(zFη(z)Fη(z))1λ=p(z(z+η)1+ηz)

    and

    (Gη(z))λ(zGη(z)Gη(z))1λ=p(z(z+η)1+ηz).

    Clearly,

    Kpn(z):={[λz0tλ1p(tn1)dt]1λ,if0<λ1,exp{z0p(tn1)dtt},ifλ=0.

    Hence, Kpn,Fη,GηN[λ,A,B]. Also, we write

    Kp2(z):={[λz0tλ1p(t)dt]1λ,if0<λ1,exp{z0p(t)dtt},ifλ=0.

    If μ<Υ1 or μ>Υ2, then the equality holds if and only if f is Kp2(z) or one of its rotations. When Υ1<μ<Υ2, then the equality holds if and only if f is Kp3(z) satisfying

    Kp3(z):={[λz0tλ1p(t2)dt]1λ,if0<λ1,exp{z0p(t2)dtt},ifλ=0

    or one of its rotations. If μ=Υ1 then the equality holds if and only if f is Fη or one of its rotations. If μ=Υ2 then the equality holds if and only if f is Gη or one of its rotations.

    As it is similar to the above result in Theorem 2.4, we state the following results without proof.

    Theorem 2.5. If the function fM[λ,A,B] is of the form (1.1) and μR, then

    |a3μa22|{8(AB)3(2λ)π2{2(B+1)π2+[4(1λ)3μ(2λ)](AB)2π2+13},(μΓ1);4(AB)3(2λ)π2,(Γ1μΓ2);8(AB)3(2λ)π2{2(B+1)π2[4(1λ)3μ(2λ)](AB)2π213},(μΓ2),

    where

    Γ1=4(1λ)3(2λ)2[π26+2(B+1)]3(2λ)(AB)

    and

    Γ2=4(1λ)3(2λ)2[5π26+2(B+1)]3(2λ)(AB).

    Further, we set

    Γ3=4(1λ)3(2λ)2[π23+2(B+1)]3(2λ)(AB).

    Then, each of the following results holds:

    (A) For μ[Γ1,Γ3],

    |a3μa22|+2π2(˜Π+12)3(2λ)(AB)|a2|24(AB)3(2λ)π2;

    (B) For μ[Γ3,Γ2],

    |a3μa22|+2π2(˜Π+12)3(2λ)(AB)|a2|24(AB)3(2λ)π2,

    where

    ˜Π=2(B+1)π2(AB)2π2[4(1λ)3μ(2λ)]13.

    Theorem 2.6. Let μR. If fA is assumed to be in W[λ,A,B], then

    |a3μa22|{4(AB)(32λ)π2{2(B+1)π2[λ2+5λ8+4μ(32λ)](AB)(2λ)2π2+13},(μ1);2(AB)(32λ)π2,(1μ2);4(AB)(32λ)π2{2(B+1)π2+[λ2+5λ8+4μ(32λ)](AB)(2λ)2π213},(μ2),

    where

    1=λ2+5λ84(32λ)[π26+2(B+1)](2λ)24(32λ)(AB)

    and

    2=λ2+5λ84(32λ)[5π26+2(B+1)](2λ)24(32λ)(AB).

    Besides, we let

    3=λ2+5λ84(32λ)[π23+2(B+1)](2λ)24(32λ)(AB).

    Then, each of the following results holds:

    (A) For μ[1,3],

    |a3μa22|+(2λ)2π2(˜Ψ+12)4(32λ)(AB)|a2|22(AB)(2+λ)π2;

    (B) For μ[3,2],

    |a3μa22|+(2λ)2π2(˜Ψ+12)4(32λ)(AB)|a2|22(AB)(2+λ)π2,

    where

    ˜Ψ=2(B+1)π2+(AB)[λ2+5λ8+4μ(32λ)](2λ)2π213.

    In this section we determine the coefficient bounds and Fekete-Szegö problems associated with logarithmic function H(z) defined by

    H(z)=logf(z)z=2n=1dnzn, (3.1)

    where the coefficient dn of H(z) is called the logarithmic coefficient of fA defined in D. Expanding (3.1) by series expansion of log(1+z) and equating the various coefficients, we assert that

    d1=a22, (3.2)
    d2=12(a3a222). (3.3)

    Theorem 3.1. Let fN[λ,A,B] with the logarithmic coefficients in (3.1), and νC. Then

    |d1|2(AB)(1+λ)π2, (3.4)
    |d2|2(AB)(2+λ)π2max{1,2|Θ|} (3.5)

    for

    Θ=2(B+1)π2+λ(2+λ)(AB)(1+λ)2π213,

    and

    |d2νd21|2(AB)(2+λ)π2max{1,2|Λ|} (3.6)

    for

    Λ=2(B+1)π2+(2+λ)(λ+ν)(AB)(1+λ)2π213.

    Proof. From (2.10) and (2.12), and (3.2) and (3.3) we get

    d1=(AB)c1(1+λ)π2,d2=(AB)(2+λ)π2[c2(16+2(B+1)π2+λ(2+λ)(AB)(1+λ)2π2)c21].

    Furthermore, we have

    d2νd21=(AB)(2+λ)π2[c2(16+2(B+1)π2+λ(2+λ)(AB)(1+λ)2π2)c21]ν((AB)c1(1+λ)π2)2=(AB)(2+λ)π2[c2ρc21], (3.7)

    where

    ρ=16+2(B+1)π2+(2+λ)(λ+ν)(AB)(1+λ)2π2.

    In view of Lemmas 1.1 and 1.2, we get the desired results such that Theorem 3.1 holds true.

    Theorem 3.2. Let fM[λ,A,B] with the logarithmic coefficients in (3.1), and νC. Then

    |d1|ABπ2, (3.8)
    |d2|2(AB)3(2λ)π2max{1,2|Ξ|} (3.9)

    for

    Ξ=2(B+1)π2+(5λ2)(AB)4π213,

    and

    |d2νd21|2(AB)3(2λ)π2max{1,2|Π|} (3.10)

    for

    Π=2(B+1)π2+[5λ+3ν(2λ)2](AB)4π213.

    Proof. According to (2.18), (2.19), (3.2) and (3.3) we get

    d1=(AB)c12π2,d2=(AB)3(2λ)π2[c2(16+2(B+1)π2+(5λ2)(AB)4π2)c21].

    Further, we have

    d2νd21=(AB)3(2λ)π2[c2(16+2(B+1)π2+(5λ2)(AB)4π2)c21]ν(AB)2c214π4=(AB)3(2λ)π2[c2ϱc21], (3.11)

    where

    ϱ=16+2(B+1)π2+[5λ+3ν(2λ)2](AB)4π2.

    Applying Lemmas 1.2 and 1.1, we obtain the desire estimates and complete the proof of Theorem 3.2.

    Theorem 3.3. Let fW[λ,A,B] with the logarithmic coefficients in (3.1), and νC. Then

    |d1|2(AB)(2λ)π2, (3.12)
    |d2|(AB)(32λ)π2max{1,2|Φ|} (3.13)

    for

    Φ=2(B+1)π2+(λ1)(λ+2)(AB)(2λ)2π213,

    and

    |d2νd21|(AB)(32λ)π2max{1,2|Ψ|} (3.14)

    for

    Ψ=2(B+1)π2+[(λ1)(λ+2)+2ν(32λ)](AB)(2λ)2π213.

    Proof. From (2.26) and (2.27), and (3.2) and (3.3) we derive

    d1=(AB)c1(2λ)π2,d2=(AB)2(32λ)π2[c2(16+2(B+1)π2+(λ1)(λ+2)(AB)(2λ)2π2)c21].

    Therefore, we obtain

    d2νd21=(AB)2(32λ)π2[c2(16+2(B+1)π2+(λ1)(λ+2)(AB)(2λ)2π2)c21]ν(AB)2c21(2λ)2π4=(AB)2(32λ)π2[c2κc21], (3.15)

    where

    κ=16+2(B+1)π2+[(λ1)(λ+2)+2ν(32λ)](AB)(2λ)2π2.

    By applying Lemmas 1.1 and 1.2, we get the desired results, which prove Theorem 3.3.

    If we consider real ν, then by Lemma 1.3 we provide the several results for Fekete-Szegö problem with respect to the logarithmic coefficients.

    Theorem 3.4. Let νR. If fN[λ,A,B] with the logarithmic coefficients is of the form (3.1), then

    |d2νd21|{4(AB)(2+λ)π2{2(B+1)π2(2+λ)(λ+ν)(AB)(1+λ)2π2+13},(ν˜Υ1);2(AB)(2+λ)π2,(˜Υ1ν˜Υ2);4(AB)(2+λ)π2{2(B+1)π2+(2+λ)(λ+ν)(AB)(1+λ)2π213},(ν˜Υ2),

    where

    ˜Υ1=λ[π26+2(B+1)](1+λ)2(2+λ)(AB)

    and

    ˜Υ2=λ[5π26+2(B+1)](1+λ)2(2+λ)(AB).

    Moreover, we put

    ˜Υ3=λ[π23+2(B+1)](1+λ)2(2+λ)(AB).

    Then, each of the following results holds:

    (i) For ν[˜Υ1,˜Υ3],

    |d2νd21|+(1+λ)2π2(Λ+12)(2+λ)(AB)|d1|22(AB)(2+λ)π2;

    (ii) For ν[˜Υ3,˜Υ2],

    |d2νd21|+(1+λ)2π2(Λ+12)(2+λ)(AB)|d1|22(AB)(2+λ)π2,

    where

    Λ=2(B+1)π2+(2+λ)(λ+ν)(AB)(1+λ)2π213.

    Theorem 3.5. Let νR. If fM[λ,A,B] with the logarithmic coefficients is of the form (3.1), then

    |d2νd21|{4(AB)3(2λ)π2{2(B+1)π2[5λ+3ν(2λ)2](AB)4π2+13},(ν˜Γ1);2(AB)3(2λ)π2,(˜Γ1ν˜Γ2);4(AB)3(2λ)π2{2(B+1)π2+[5λ)+3ν(2λ)2](AB)4π213},(ν˜Γ2),

    where

    ˜Γ1=5λ23(2λ)4[π26+2(B+1)]3(2λ)(AB)

    and

    ˜Γ2=5λ23(2λ)4[5π26+2(B+1)]3(2λ)(AB).

    Moreover, we put

    ˜Γ3=5λ23(2λ)4[π23+2(B+1)]3(2λ)(AB).

    Then, each of the following results holds:

    (i) For ν[˜Γ1,˜Γ3],

    |d2νd21|+4π2(Π+12)3(2λ)(AB)|d1|22(AB)3(2λ)π2;

    (ii) For ν[˜Γ3,˜Γ2],

    |d2νd21|+4π2(Π+12)3(2λ)(AB)|d1|22(AB)3(2λ)π2,

    where

    Π=2(B+1)π2+[5λ+3ν(2λ)2](AB)4π213.

    Theorem 3.6. Let νR. If fW[λ,A,B] with the logarithmic coefficients is of the form (3.1), then

    |d2νd21|{2(AB)(32λ)π2{2(B+1)π2[(λ+1)(λ+2)+2ν(32λ)](AB)(2λ)2π2+13},(ν˜1);(AB)(32λ)π2,(˜1ν˜2);2(AB)(32λ)π2{2(B+1)π2+[(λ+1)(λ+2)+2ν(32λ)](AB)(2λ)2π213},(ν˜2),

    where

    ˜1=(λ+1)(λ+2)2(32λ)[π26+2(B+1)](2λ)22(32λ)(AB)

    and

    ˜2=(λ2+1)(λ+2)2(32λ)[5π26+2(B+1)](2λ)22(32λ)(AB).

    Moreover, we let

    ˜3=(λ2+1)(λ+2)2(32λ)[π23+2(B+1)](2λ)22(32λ)(AB).

    Then, each of the following results holds:

    (i) For μ[˜1,˜3],

    |d2νd21|+(2λ)2π2(Ψ+12)2(32λ)(AB)|d1|2(AB)(32λ)π2;

    (ii) For ν[˜3,˜2],

    |d2νd21|+(2λ)2π2(Ψ+12)2(32λ)(AB)|d1|2(AB)(32λ)π2,

    where

    Ψ=2(B+1)π2+[(λ1)(λ+2)+2ν(32λ)](AB)(2λ)2π213.

    Concluding Remark: By fixing A=1andB=1 or A=1andB=12α, one can deduce some interesting results.

    The authors are profoundly grateful to all the reviewers for their careful readings and insightful suggestions such that the original manuscript for this article is greatly improved.

    This work is supported by Natural Science Foundation of Ningxia (Grant No. 2020AAC03066) and Natural Science Foundation of China (Grant Nos. 42064004; 11762017).

    The authors declare no conflict of interest.



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