Research article Special Issues

Multi-fractional-differential operators for a thermo-elastic magnetic response in an unbounded solid with a spherical hole via the DPL model

  • Received: 23 October 2022 Revised: 20 November 2022 Accepted: 20 November 2022 Published: 20 December 2022
  • MSC : 35B40, 35Q79, 35J55, 45F15, 73B30

  • The current research aims to investigate thermodynamic responses to thermal media based on a modified mathematical model in the field of thermoelasticity. In this context, it was considered to present a new model with a fractional time derivative that includes Caputo-Fabrizio and Atangana-Baleanu fractional differential operators within the framework of the two-phase delay model. The proposed mathematical model is employed to examine the problem of an unbounded material with a spherical hole experiencing a reduced moving heat flow on its inner surface. The problem is solved analytically within the modified space utilizing the Laplace transform as the solution mechanism. An arithmetic inversion of the Laplace transform was performed and presented visually and tabularly for the studied distributions. In the tables, specific comparisons are introduced to evaluate the influences of different fractional operators and thermal properties on the response of all the fields examined.

    Citation: Osama Moaaz, Ahmed E. Abouelregal. Multi-fractional-differential operators for a thermo-elastic magnetic response in an unbounded solid with a spherical hole via the DPL model[J]. AIMS Mathematics, 2023, 8(3): 5588-5615. doi: 10.3934/math.2023282

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  • The current research aims to investigate thermodynamic responses to thermal media based on a modified mathematical model in the field of thermoelasticity. In this context, it was considered to present a new model with a fractional time derivative that includes Caputo-Fabrizio and Atangana-Baleanu fractional differential operators within the framework of the two-phase delay model. The proposed mathematical model is employed to examine the problem of an unbounded material with a spherical hole experiencing a reduced moving heat flow on its inner surface. The problem is solved analytically within the modified space utilizing the Laplace transform as the solution mechanism. An arithmetic inversion of the Laplace transform was performed and presented visually and tabularly for the studied distributions. In the tables, specific comparisons are introduced to evaluate the influences of different fractional operators and thermal properties on the response of all the fields examined.



    In his survey-cum-expository review article, Srivastava [1] presented and motivated about brief expository overview of the classical q -analysis versus the so-called (p,q)-analysis with an obviously redundant additional parameter p. We also briefly consider several other families of such extensively and widely-investigated linear convolution operators as (for example) the Dziok-Srivastava, Srivastava-Wright and Srivastava-Attiya linear convolution operators, together with their extended and generalized versions. The theory of (p,q)-analysis has important role in many areas of mathematics and physics. Our usages here of the q-calculus and the fractional q-calculus in geometric function theory of complex analysis are believed to encourage and motivate significant further developments on these and other related topics (see Srivastava and Karlsson [2,pp. 350-351], Srivastava [3,4]). Our main objective in this survey-cum-expository article is based chiefly upon the fact that the recent and future usages of the classical q-calculus and the fractional q-calculus in geometric function theory of complex analysis have the potential to encourage and motivate significant further researches on many of these and other related subjects. Jackson [5,6] was the first that gave some application of q -calculus and introduced the q-analogue of derivative and integral operator (see also [7,8]), we apply the concept of q -convolution in order to introduce and study the general Taylor-Maclaurin coefficient estimates for functions belonging to a new class of normalized analytic in the open unit disk, which we have defined here.

    Let A denote the class of analytic functions of the form

    f(z):=z+m=2amzm,zΔ:={zC:|z|<1} (1.1)

    and let SA consisting on functions that are univalent in Δ. If the function hA is given by

    h(z):=z+m=2bmzm,(zΔ).                                  (1.2)

    The Hadamard product (or convolution) of f and h, given by (1.1) and (1.2), respectively, is defined by

    (fh)(z):=z+m=2ambmzm,zΔ. (1.3)

    If f and F are analytic functions in Δ, we say that f is subordinate to F, written as f(z)F(z), if there exists a Schwarz function s, which is analytic in Δ, with s(0)=0, and |s(z)|<1 for all zΔ, such that f(z)=F(s(z)), zΔ. Furthermore, if the function F is univalent in Δ, then we have the following equivalence ([9,10])

    f(z)F(z)f(0)=F(0)andf(Δ)F(Δ).

    The Koebe one-quarter theorem (see [11]) prove that the image of Δ under every univalent function fS contains the disk of radius 14. Therefore, every function fS has an inverse f1 that satisfies

    f(f1(w))=w,(|w|<r0(f),r0(f)14),

    where

    g(w)=f1(w)=wa2w2+(2a22a3)w3(5a325a2a3+a4)w4+.=w+m=2Amwm

    A function fA is said to be bi-univalent in Δ if both f and f1 are univalent in Δ. Let Σ represent the class of bi-univalent functions in Δ given by (1.1). The class of analytic bi-univalent functions was first familiarised by Lewin [12], where it was shown that |a2|<1.51. Brannan and Clunie [13] enhanced Lewin's result to |a2|<2 and later Netanyahu [14] proved that |a2|<43. 

    Note that the functions

    f1(z)=z1z,f2(z)=12log1+z1z,f3(z)=log(1z)

    with their corresponding inverses

    f11(w)=w1+w,f12(w)=e2w1e2w+1,f13(w)=ew1ew

    are elements of Σ (see [15,16]). For a brief history and exciting examples in the class Σ (see [17]). Brannan and Taha [18] (see also [16]) presented certain subclasses of the bi-univalent functions class Σ similar to the familiar subclasses S(α) and K(α) of starlike and convex functions of order α (0α<1), respectively (see [17,19,20]). Ensuing Brannan and Taha [18], a function fA is said to be in the class SΣ(α) of bi-starlike functions of order α (0<α1), if each of the following conditions are satisfied:

    fΣ,with|argzf(z)f(z)|<απ2(zΔ),

    and

    |argwg(w)g(w)|<απ2(wΔ),

    where the function g is the analytic extension of f1 to Δ, given by

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

    A function fA is said to be in the class KΣ(α) of bi-convex functions of order α (0<α1), if each of the following conditions are satisfied:

    fΣ,with|arg(1+zf(z)f(z))|<απ2(zΔ),

    and

    |arg(1+wg(w)g(w))|<απ2(wΔ).

    The classes SΣ(α) and KΣ(α) of bi-starlike functions of order α and bi-convex functions of order α (0<α1), corresponding to the function classes S(α) and K(α), were also introduced analogously. For each of the function classes SΣ(α) and KΣ(α), they found non-sharp estimates on the first two Taylor-Maclaurin coefficients |a2| and |a3| ([16,18]).

    The Faber polynomials introduced by Faber [21] play an important role in various areas of mathematical sciences, especially in Geometric Function Theory of Complex Analysis (see, for details, [22]). In 2013, Hamidi and Jahangiri [23,24,25] took a new approach to show that the initial coefficients of classes of bi- starlike functions e as well as provide an estimate for the general coefficients of such functions subject to a given gap series condition.Recently, their idea of application of Faber polynomials triggered a number of related publications by several authors (see, for example, [26,27,28] and also references cited threin) investigated some interesting and useful properties for analytic functions. Using the Faber polynomial expansion of functions fA has the form (1.1), the coefficients of its inverse map may be expressed as

    g(w)=f1(w)=w+m=21mKmm1(a2,a3,...)wm, (1.5)

    where

    Kmm1(a2,a3,...)=(m)!(2m+1)!(m1)!am12+(m)!(2(m+1))!(m3)!am32a3+(m)!(2m+3)!(m4)!am42a4+(m)!(2(m+2))!(m5)!am52[a5+(m+2)a23]+(m)!(2m+5)!(m6)!am62[a6+(2m+5)a3a4]+i7ami2Ui, (1.6)

    such that Ui with 7im is a homogeneous polynomial in the variables a2,a3,...,am, In particular, the first three terms of Kmm1 are

    K21=2a2,K32=3(2a22a3),K43=4(5a325a2a3+a4).

    In general, an expansion of Knm (nN) is (see [29,30,31,32,33])

    Knm=nam+n(n1)2D2m+n!3!(n3)!D3m+...+n!m!(nm)!Dmm,

    where Dnm=Dnm(a2,a3,...) and

    Dpm(a1,a2,...am)=m=1p!i1!...im!ai11...aimm,

    while a1=1 and the sum is taken over all non-negative integers i1...im satisfying

    i1+i2+...+im=pi1+2i2+...+mim=m.

    Evidently

    Dmm(a1,a2,...am)=am1.

    Srivastava [1] made use of several operators of q-calculus and fractional q-calculus and recollecting the definition and representations. The q-shifted factorial is defined for κ,qC and nN0=N{0} as follows

    (κ;q)m={1,m=0(1κ)(1κq)(1κqk1),mN.

    By using the q-Gamma function Γq(z), we get

    (qκ;q)m=(1q)m Γq(κ+m)Γq(κ)(mN0),

    where (see [34])

    Γq(z)=(1q)1z(q;q)(qz;q)(|q|<1).

    Also, we note that

    (κ;q)=m=0(1κqm)(|q|<1),

    and, the q-Gamma function Γq(z) is known

    Γq(z+1)=[z]q Γq(z),

    where [m]q symbolizes the basic q-number defined as follows

    [m]q:={1qm1q,mC1+m1j=1qj,mN. (1.7)

    Using the definition formula (1.7) we have the next two products:

    (i) For any non-negative integer m, the q-shifted factorial is given by

    [m]q!:={1,ifm=0,mn=1[n]q,  ifmN.

    (ii) For any positive number r, the q-generalized Pochhammer symbol is defined by

    [r]q,m:={1,ifm=0,r+m1n=r[n]q,ifmN.

    It is known in terms of the classical (Euler's) Gamma function Γ(z), that

    Γq(z)Γ(z)     asq1.

    Also, we observe that

    limq1{(qκ;q)m(1q)m}=(κ)m,

    where (κ)m is the familiar Pochhammer symbol defined by

    (κ)m={1,ifm=0,κ(κ+1)...(κ+m1),ifmN.

    For 0<q<1, the q-derivative operator (or, equivalently, the q- difference operator) El-Deeb et al. [35] defined Dq for fh given by (1.3) is defined by (see [5,6])

    Dq(fh)(z):=Dq(z+m=2ambmzm)=(fh)(z)(fh)(qz)z(1q)=1+m=2[m]qambmzm1(zΔ),

    where, as in the definition (1.7)

    [m]q:={1qm1q=1+m1j=1qj      (mN),0                               (m=0). (1.8)

    For κ>1 and 0<q<1, El-Deeb et al. [35] (see also) defined the linear operator Hκ,qh:AA by

    Hκ,qhf(z)Mq,κ+1(z)=zDq(fh)(z)(zΔ),

    where the function Mq,κ+1 is given by

    Mq,κ+1(z):=z+m=2[κ+1]q,m1[m1]q!zm(zΔ).

    A simple computation shows that

    Hκ,qhf(z):=z+m=2[m]q![κ+1]q,m1ambm zm(κ>1,0<q<1, zΔ). (1.9)

    From the definition relation (1.9), we can easily verify that the next relations hold for all fA:

    (i) [κ+1]qHκ,qhf(z)=[κ]qHκ+1,qhf(z)+qκz Dq(Hκ+1,qhf(z))(zΔ);(ii)Iκhf(z):=limq1Hκ,qhf(z)=z+m=2m!(κ+1)m1ambmzm(zΔ). (1.10)

    Remark 1. Taking precise cases for the coefficients bm we attain the next special cases for the operator Hκ,qh:

    (ⅰ) For bm=1, we obtain the operator Iκq defined by Srivastava [32] and Arif et al. [36] as follows

    Iκqf(z):=z+m=2[m]q![κ+1]q,m1amzm(κ>1,0<q<1, zΔ); (1.11)

    (ⅱ) For bm=(1)m1Γ(υ+1)4m1(m1)!Γ(m+υ), υ>0, we obtain the operator Nκυ,q defined by El-Deeb and Bulboacă [37] and El-Deeb [38] as follows

    Nκυ,qf(z):=z+m=2(1)m1Γ(υ+1)4m1(m1)!Γ(m+υ)[m]q![κ+1]q,m1amzm=z+m=2[m]q![κ+1]q,m1ψmamzm(υ>0,κ>1,0<q<1, zΔ), (1.12)

    where

    ψm:=(1)m1Γ(υ+1)4m1(m1)!Γ(m+υ); (1.13)

    (ⅲ) For bm=(n+1n+m)α, α>0, n0, we obtain the operator Mκ,αn,q defined by El-Deeb and Bulboacă [39] and Srivastava and El-Deeb [40] as follows

    Mκ,αn,qf(z):=z+m=2(n+1n+m)α[m]q![κ+1]q,m1amzm(zΔ); (1.14)

    (ⅳ) For bm=ρm1(m1)!eρ, ρ>0, we obtain the q-analogue of Poisson operator defined by El-Deeb et al. [35] (see [41]) as follows

    Iκ,ρqf(z):=z+m=2ρm1(m1)!eρ[m]q![κ+1]q,m1amzm(zΔ). (1.15)

    (ⅴ) For bm=[1++μ(m1)1+]n, nZ, 0, μ0, we obtain the q-analogue of Prajapat operator defined by El-Deeb et al. [35] (see also [42]) as follows

    Jκ,nq,,μf(z):=z+m=2[1++μ(m1)1+]n[m,q]![κ+1,q]m1amzm(zΔ); (1.16)

    (ⅵ) For bm=(n+m2m1)θm1(1θ)n nN, 0θ1, we obtain the q-analogue of the Pascal distribution operator defined by Srivastava and El-Deeb [28] (see also [35,43,44]) as follows

    κ,nq,θf(z):=z+m=2(n+m2m1)θm1(1θ)n[m,q]![κ+1,q]m1amzm(zΔ). (1.17)

    The purpose of the paper is to present a new subclass of functions Lq,κΣ(η;h;Φ) of the class Σ, that generalize the previous defined classes. This subclass is defined with the aid of a general Hκ,qh linear operator defined by convolution products composed with the aid of q-derivative operator. This new class extend and generalize many preceding operators as it was presented in Remark 1, and the main goal of the paper is find estimates on the coefficients |a2|, |a3|, and for the Fekete-Szegö functional for functions in these new subclasses. These classes will be introduced by using the subordination and the results are obtained by employing the techniques used earlier by Srivastava et al. [16]. This last work represents one of the most important study of the bi-univalent functions, and inspired many investigations in this area including the present paper, while many other recent papers deals with problems initiated in this work, like [33,44,45,46,47,48], and many others. Inspired by the work of Silverman and Silvia [49] (also see[50]) and recent study by Srivastava et al [51], in this article, we define the following new subclass of bi-univalent functions Mq,κΣ(ϖ,ϑ,h) as follows:

    Definition 1. Let ϖ(π,π] and let the function fΣ be of the form (1.1) and h is given by (1.2), the function f is said to be in the class Mq,κΣ(ϖ,ϑ,h) if the following conditions are satisfied:

    ((Hκ,qhf(z))+(1+eiϖ)2z(Hκ,qhf(z)))>ϑ, (1.18)

    and

    ((Hκ,qhg(w))+(1+eiϖ)2w(Hκ,qhg(w)))>ϑ (1.19)

    with κ>1, 0<q<1, 0ϑ<1 and z,wΔ, where the function g is the analytic extension of f1 to Δ, and is given by (1.4).

    Definition 2. Let ϖ=0 and let the function fΣ be of the form (1.1) and h is given by (1.2), the function f is said to be in the class Mq,κΣ(ϑ,h) if the following conditions are satisfied:

    ((Hκ,qhf(z))+z(Hκ,qhf(z)))>ϑ, (1.20)

    and

    ((Hκ,qhg(w))+w(Hκ,qhg(w)))>ϑ (1.21)

    with κ>1, 0<q<1, 0ϑ<1 and z,wΔ, where the function g is the analytic extension of f1 to Δ, and is given by (1.4).

    Definition 3. Let ϖ=π and let the function fΣ be of the form (1.1) and h is given by (1.2), the function f is said to be in the class HMq,κΣ(ϑ,h) if the following conditions are satisfied:

    ((Hκ,qhf(z)))>ϑand((Hκ,qhg(w)))>ϑ (1.22)

    with κ>1, 0<q<1, 0ϑ<1 and z,wΔ, where the function g is the analytic extension of f1 to Δ, and is given by (1.4).

    Remark 2. (ⅰ) Putting q1 we obtain that limq1Mq,κΣ(ϖ,ϑ;h)=:GκΣ(ϖ,ϑ;h), where GκΣ(ϖ,ϑ;h) represents the functions fΣ that satisfy (1.18) and (1.19) for Hκ,qh replaced with Iκh (1.10).

    (ⅱ) Fixing bm=(1)m1Γ(υ+1)4m1(m1)!Γ(m+υ), υ>0, we obtain the class Bq,κΣ(ϖ,ϑ,υ), that represents the functions fΣ that satisfy (1.18) and (1.19) for Hκ,qh replaced with Nκυ,q (1.12).

    (ⅲ) Taking bm=(n+1n+m)α, α>0, n0, we obtain the class Lq,κΣ(ϖ,ϑ,n,α), that represents the functions fΣ that satisfy (1.18) and (1.19) for Hκ,qh replaced with Mκ,αn,q (1.14).

    (ⅳ) Fixing bm=ρm1(m1)!eρ, ρ>0, we obtain the class Mq,κΣ(ϖ,ϑ,ρ), that represents the functions fΣ that satisfy (1.18) and (1.19) for Hκ,qh replaced with Iκ,ρq (1.15).

    (ⅴ) Choosing bm=[1++μ(m1)1+]n, nZ, 0, μ0, we obtain the class Mq,κΣ(ϖ,ϑ,n,,μ), that represents the functions fΣ that satisfy (1.18) and (1.19) for Hκ,qh replaced with Jκ,nq,,μ (1.16).

    Throughout this paper, we assume that

    ϖ(π;π],κ>1,0ϑ<1,0<q<1.

    Recall the following Lemma which will be needed to prove our results.

    Lemma 1. (Caratheodory Lemma [11]) If ϕP and ϕ(z)=1+n=1cnzn then |cn|2 for each n, this inequality is sharp for all n where P is the family of all functions ϕ analytic and having positive real part in Δ with ϕ(0)=1.

    We firstly introduce a bound for the general coefficients of functions belong to the class Mq,κΣ(ϖ,ϑ;h).

    Theorem 2. Let the function f given by (1.1) belongs to the class Mq,κΣ(ϖ,ϑ;h). If ak=0 for 2km1, then

    |am|4(1ϑ)[κ+1,q]m1m|2+(1+eiϖ)(m1)| [m,q]!bm.

    Proof. If fMq,κΣ(ϖ,ϑ;h), from (1.18), (1.19), we have

    ((Hκ,qhf(z))+(1+eiϖ)2z(Hκ,qhf(z)))=1+m=2m2[2+(1+eiϖ)(m1)][m,q]![κ+1,q]m1bmamzm1(zΔ), (2.1)

    and

    ((Hκ,qhg(w))+(1+eiϖ)2z(Hκ,qhg(w)))=1+m=2m2[2+(1+eiϖ)(m1)][m,q]![κ+1,q]m1bm Amwm1
    =1+m=2m2[2+(1+eiϖ)(m1)][m,q]![κ+1,q]m1bm 1mKmm1(a2,...,am)wm1(wΔ). (2.2)

    Since

    fMq,κΣ(ϖ,ϑ;h) and g=f1Mq,κΣ(γ,η,ϑ;h),

    we know that there are two positive real part functions:

    U(z)=1+m=1cmzm,

    and

    V(w)=1+m=1dmwm,

    where

    (U(z))>0and (V(w))>0(z,wΔ),

    so that

    (Hκ,qhf(z))+(1+eiθ)2z(Hκ,qhf(z))=ϑ+(1ϑ)U(z)
    =1+(1ϑ)m=1cmzm, (2.3)

    and

    (Hκ,qhg(w))+(1+eiθ)2z(Hκ,qhg(w))=ϑ+(1ϑ)V(w)
    =1+(1ϑ)m=1dmwm. (2.4)

    Using (2.1) and comparing the corresponding coefficients in (2.3), we obtain

    m2[2+(1+eiϖ)(m1)][m,q]![κ+1,q]m1bmam=(1ϑ)cm1, (2.5)

    and similarly, by using (2.2) in the equality (2.4), we have

    m2[2+(1+eiϖ)(m1)][m,q]![κ+1,q]m1bm1mKmm1(a2,a3,...am)=(1ϑ)dm1, (2.6)

    under the assumption ak=0 for 0km1, we obtain Am=am and so

    m2[2+(1+eiϖ)(m1)][m,q]![κ+1,q]m1bmam=(1ϑ)cm1, (2.7)

    and

    m2[2+(1+eiϖ)(m1)][m,q]![κ+1,q]m1bmam=(1ϑ)dm1, (2.8)

    Taking the absolute values of (2.7) and (2.8), we conclude that

    |am|=|2(1ϑ)[κ+1,q]m1cm1m[2+(1+eiϖ)(m1)] [m,q]!bm|=|2(1ϑ)[κ+1,q]m1dm1m[2+(1+eiϖ)(m1)] [m,q]!bm|.

    Applying the Caratheodory Lemma 1, we obtain

    |am|4(1ϑ)[κ+1,q]m1m|2+(1+eiϖ)(m1)| [m,q]!bm,

    which completes the proof of Theorem.

    Theorem 3. Let the function f given by (1.1) belongs to the class Mq,κΣ(ϖ,ϑ;h), then

    |a2|{2(1ϑ)[κ+1,q]|3+eiϖ|[2,q]!b2,0ϑ<1|3+eiϖ|2 ([2,q]!)2[κ+2,q]b223|2+eiϖ| [3,q]![κ+1,q]b32(1ϑ)[κ+1,q]23|2+eiϖ| [3,q]!b3,1|3+eiϖ|2 ([2,q]!)2[κ+2,q]b223|2+eiϖ| [3,q]![κ+1,q]b3ϑ<1, (2.9)
    |a3|2(1ϑ)[κ+1,q]23|2+eiϖ|[3,q]!b3, (2.10)

    and

    |a32a22|2(1ϑ)[κ+1,q]23|2+eiϖ| [3,q]!b3. (2.11)

    Proof. Fixing m=2 and m=3 in (2.5), (2.6), we have

    (3+eiϖ) [2,q]![κ+1,q]b2a2=(1ϑ)c1, (2.12)
    3(2+eiϖ) [3,q]![κ+1,q]2b3a3=(1ϑ)c2, (2.13)
    (3+eiϖ) [2,q]![κ+1,q]b2a2=(1ϑ)d1, (2.14)

    and

    3(2+eiϖ) [3,q]![κ+1,q]2b3(2a22a3)=(1ϑ)d2. (2.15)

    From (2.12) and (2.14), by using the Caratheodory Lemma1, we obtain

    |a2|=(1ϑ)[κ+1,q]|c1||3+eiϖ|[2,q]!b2=(1ϑ)[κ+1,q]|d1||3+eiϖ|[2,q]!b22(1ϑ)[κ+1,q]|3+eiϖ|[2,q]!b2. (2.16)

    Also, from (2.13) and (2.15), we have

    6(2+eiϖ) [3,q]![κ+1,q]2b3a22=(1ϑ)(c2+d2),
     a22=(1ϑ)[κ+1,q]26(2+eiϖ)[3,q]!b3(c2+d2), (2.17)

    and by using the Caratheodory Lemma 1, we obtain

    |a2|2(1ϑ)[κ+1,q]23|2+eiϖ| [3,q]!b3. (2.18)

    From (2.16) and (2.18), we obtain the desired estimate on the coefficient as asserted in (2.9).

    To find the bound on the coefficient |a3|, we subtract (2.15) from (2.13). we get

    6(2+eiϖ) [3,q]![κ+1,q]2b3(a3a22)=(1ϑ)(c2d2),

    or

    a3=a22+(1ϑ)(c2d2)[κ+1,q]26(2+eiϖ)[3,q]!b3, (2.19)

    substituting the value of a22 from (2.12) into (2.19), we obtain

    a3=(1ϑ)2[κ+1,q]2c21(3+eiϖ)2([2,q]!)2b22+(1ϑ)(c2d2)[κ+1,q]26(2+eiϖ)[3,q]!b3.

    Using the Caratheodory Lemma 1, we find that

    |a3|4(1ϑ)2[κ+1,q]2|3+eiϖ|2([2,q]!)2b22+2(1ϑ)[κ+1,q]23|2+eiϖ|[3,q]!b3, (2.20)

    and from (2.13), we have

    a3=(1ϑ)[κ+1,q]2 c23(2+eiϖ)[3,q]!b3.

    Appling the Caratheodory Lemma 1, we obtain

    |a3|2(1ϑ)[κ+1,q]23|2+eiϖ|[3,q]!b3. (2.21)

    Combining (2.20) and (2.21), we have the desired estimate on the coefficient |a3| as asserted in (2.10).

    Finally, from (2.15), we deduce that

    |a32a22|(1ϑ)[κ+1,q]2|d2|3|2+eiϖ| [3,q]!b3=2(1ϑ)[κ+1,q]23|2+eiϖ| [3,q]!b3.

    Thus the proof of Theorem 3 was completed.

    Fekete and Szegö [52] introduced the generalized functional |a3a22|, where is some real number. Due to Zaprawa [53], (also see [54]) in the following theorem we determine the Fekete-Szegö functional for fMq,κΣ(ϖ,ϑ;h).

    Theorem 4. Let the function f given by (1.1) belongs to the class Mq,κΣ(ϖ,ϑ;h) and R. Then we have

    |a3a22|((1ϑ)[κ+1,q]23|2+eiϖ|[3,q]!b3){|2|+||}.

    Proof. From (2.17) and (2.19)we obtain

    a3a22=(1)(1ϑ)[κ+1,q]26(2+eiϖ)[3,q]!b3(c2+d2)+(1ϑ)[κ+1,q]26(2+eiϖ)[3,q]!b3(c2d2),=((1ϑ)[κ+1,q]26(2+eiϖ)[3,q]!b3){[(1)+1]c2+[(1)1]d2}.

    So we have

    a3a22=((1ϑ)[κ+1,q]26(2+eiϖ)[3,q]!b3){(2)c2+()d2}. (3.1)

    Then, by taking modulus of (3.1), we conclude that

    |a3a22|((1ϑ)[κ+1,q]23|2+eiϖ|[3,q]!b3){|2|+||}

    Taking =1, we have the following result.

    |a3a22|2(1ϑ)[κ+1,q]23|2+eiϖ|[3,q]!b3.

    In the current paper, we mainly get upper bounds of the initial Taylors coefficients of bi-univalent functions related with q calculus operator. By fixing bm as demonstrated in Remark 1, one can effortlessly deduce results correspondents to Theorems 2 and 3 associated with various operators listed in Remark 1. Further allowing q1 as itemized in Remark 2 we can outspread the results for new subclasses stated in Remark 2. Moreover by fixing ϖ=0 and ϖ=π in Theorems 2 and 3, we can easily state the results for fMq,κΣ(ϑ;h) and fHMq,κΣ(ϑ;h). Further by suitably fixing the parameters in Theorem 4, we can deduce Fekete-Szegö functional for these function classes. By using the subordination technique, we can extend the study by defining a new class

    [(Hκ,qhf(z))+(1+eiϖ2)z(Hκ,qhf(z))]Ψ(z)

    where Ψ(z) the function Ψ is an analytic univalent function such that (Ψ)>0inΔ with Ψ(0)=1,Ψ(0)>0 and Ψ maps Δ onto a region starlike with respect to 1 and symmetric with respect to the real axis and is given by Ψ(z)=z+B1z+B2z2+B3z3+,(B1>0). Also, motivating further researches on the subject-matter of this, we have chosen to draw the attention of the interested readers toward a considerably large number of related recent publications (see, for example, [1,2,4]). and developments in the area of mathematical analysis. In conclusion, we choose to reiterate an important observation, which was presented in the recently-published review-cum-expository review article by Srivastava ([1], p. 340), who pointed out the fact that the results for the above-mentioned or new q analogues can easily (and possibly trivially) be translated into the corresponding results for the so-called (p;q)analogues(with 0<|q|<p1)by applying some obvious parametric and argument variations with the additional parameter p being redundant.

    The researcher(s) would like to thank the Deanship of Scientific Research, Qassim University for funding the publication of this project.The authors are grateful to the reviewers for their valuable remarks, comments, and advices that help us to improve the quality of the paper.

    The authors declare that they have no competing interests.



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