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Research article Special Issues

Matrix-Valued hypergeometric Appell-Type polynomials


  • In recent years, much attention has been paid to the role of special matrix polynomials of a real or complex variable in mathematical physics, especially in boundary value problems. In this article, we define a new type of matrix-valued polynomials, called the first Appell matrix polynomial of two complex variables. The properties of the newly definite matrix polynomial involving, generating matrix functions, recurrence relations, Rodrigues' type formula and integral representation are investigated. Further, relevant connections between the first Appell matrix polynomial and various matrix functions are reported. The current study may open the door for further investigations concerning the practical applications of matrix polynomials associated with a system of differential equations.

    Citation: Muajebah Hidan, Ahmed Bakhet, Hala Abd-Elmageed, Mohamed Abdalla. Matrix-Valued hypergeometric Appell-Type polynomials[J]. Electronic Research Archive, 2022, 30(8): 2964-2980. doi: 10.3934/era.2022150

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  • In recent years, much attention has been paid to the role of special matrix polynomials of a real or complex variable in mathematical physics, especially in boundary value problems. In this article, we define a new type of matrix-valued polynomials, called the first Appell matrix polynomial of two complex variables. The properties of the newly definite matrix polynomial involving, generating matrix functions, recurrence relations, Rodrigues' type formula and integral representation are investigated. Further, relevant connections between the first Appell matrix polynomial and various matrix functions are reported. The current study may open the door for further investigations concerning the practical applications of matrix polynomials associated with a system of differential equations.



    In 1880, Appell introduced in [1] sequences of polynomials {Pn(η)}n0 satisfying the relation

    ddηPn(η)=nPn1(η),P0(η)0.

    If P(τ) is a formal power series of the form

    P(τ)=n=0anτnn!,a00,

    Then Appell sequences can also be defined by means of their exponential generating function G(η,τ) given by

    G(η,τ)=P(τ)eητ=n=0Pn(η)τnn!.

    Several members belonging to the Appell family can be obtained by properly choosing P(τ), such as Bernoulli polynomials, Euler polynomials, hypergeometric Bernoulli polynomials, Genocchi polynomials and Hermit polynomials (cf. [2]).

    In [3], the new Appell polynomial family Akn(m,η) are presented in the terms of the generalized hypergeometric function as follows

    Akn(m,η)=ηnk+pFq[α1,α2,...,αp,nk,n1k,...,nk+1kβ1,β2,.....,βq;mηk],

    where the generalized hypergeometric function is written in the following manner

    pFq[α1α2αpβ1β2βq;η]=n=0(α1)n(αp)n(β1)n(βq)nηnn!ηC,

    and α1,αp are complex parameters with β1,βpCZ0 (Z0={0}Z), and

    (α1)=Γ(α1+)Γ(α1)={α1(α1+1)...(α1+1),N,α1C1,=0;ϑ1C{0}, (1.1)

    is the Pochhammer symbol and Γ(.) is gamma function.

    The class of Gauss hypergeometric polynomials is defined by Bajpai and Arora [4] in the following equivalent formulas

    Aϑ2,ϑ3n(ξ)=ξn2F1(n,ϑ2ϑ3;1ξ)(nN0={0}N)=(ϑ2)n(ϑ3)n2F1(n,1ϑ3n1ϑ2n;ξ). (1.2)

    Also, the authors [4] investigated several results of the polynomials Aα,βn(ξ) included, semi-orthogonality, integral formulas, finite sums and some relevant connection with Foxs H-function and Jacobi polynomials. Moreover, generating function and orthogonality property of a class of of Gauss hypergeometric polynomials occurring in quantum mechanics presented by Bajpai in [5]. Khanna and Srinivasa Bhagavan [6] derived the generating function of Aα,βn(ξ) using the representations of the Lie group SL(2,C). However, mathemtical proplerties of generalized hypergeometric polynomial are reported by Khan [8]. Morover, A new real-valued Appell-type polynomial family by mean of a generalized hypergeometric function are presented by Bedratyuk and Luno [7]. Further, some finite summation formulas involving multivariable hypergeometric polynomials are archived by Djordjevic et al. [9]. Additionaly, the zeros of a class of generalized hypergeometric polynomials with applications are investegated in [10,11]. Furthermore, Appell polynomials turn into the Gould-Hopper polynomials in [12]. Later, Çekim and Aktaş [13] introduced the matrix generalization of the Gould-Hopper polynomials by means of the generating function. Recently, the Gould-Hopper-Laguerre-Appell matrix polynomials using operational methods and to investigate their properties are introduced by Nahid and Khan [14]. More recent, they are derived the matrix recurrence relations, the matrix differential, matrix integro-differential and matrix partial differential equations for the Gould-Hopper-Laguerre-Appell matrix polynomials in [15]. In a similar vein, Defez et al. presented Bernoulli matrix polynomials and discussed some its properties in [16].

    In recent years, a prominent study problem that gained attraction is matrix-valued polynomials and their applications (see, e.g., [17,18,19]). Matrix-valued Gegenbauer-type polynomials and their applications are discussed by Koelink et al. [20]. While Ismail et al. [21], presented matrix valued Hermite polynomials and some properties. Further, results on Jacobi, Gegenbauer, Legendre, generalized Bessel and Laguerre matrix polynomials have been archived in [22]. Later on, the researchers in [23] established some results on the two complex variables first Appell hypergeometric matrix function F1 considering the convergence domain {(z,w),C2:|z|<1,|w|<1}. They derived new formulas involving the contiguous relations, finite sums, the generating matrix functions, and several recursion formulae.

    The purpose of the current manuscript is to introduce a new matrix-valued Appell-type polynomial by using first Appell hypergeometric matrix function F1 and discuss certain mathematical properties for the novel defined matrix polynomial.

    The paper is organized as follows. First, in Section 2, some basic concepts and and notations needed in the results are recorded. In Section 3, we introduce the first appell matrix polynomial in terms of the first Appell hypergeometric matrix function F1 and discusses some limit formulas and auxiliary matrix polynomials of the first appell matrix polynomial. In Section 4, we prove some different generating matrix functions for the first appell matrix polynomials. Section 5 explore different recurrence relations to simplify the computation of the first appell matrix polynomials. We establish in Section 6 Rodrigues' type formula for the first appell matrix polynomial. Certain integral representation for the first appell matrix polynomial is derived in Section 7. Matrix partial differential equations satisfied by the first appell matrix polynomial in Section 8. Finally, in Section 9, we shows the concluding remarks.

    Here, we will summarize basic concepts and notations that will be largely exploited in this work (see, e.g., [17,18,22]).

    Let Mj(C) denotes the complex vector space constituted of all square matrices with j rows and j columns with entries in complex space. For any matrix TMj(C), σ(T) (spectrum of T) denotes the set of all eigenvalues of T,

    μ(T)=max{(η):ησ(T)},˜μ(T)=min{(η):ησ(T)}, (2.1)

    where μ(T) is referred to as the spectral abscissa (the largest of the real parts of its eigenvalues) and μ(T)=˜μ(T). The square matrix T is said to be positive stable if and only if ˜μ(T)>0. I and 0 stand for the identity matrix and the zero matrix in Mj(C), respectively.

    If Φ1(η) and Φ2(η) are holomorphic functions of the complex variable z, which are defined in an open set Ω of the complex plane, and T is a matrix in Mj(C) with σ(T)Ω, then from the properties of the matrix functional calculus, ([18]) we have

    Θ1(T)Θ2(T)=Θ2(T)Θ1(T).

    If R,T in Mj(C) and RT=TR, then

    Θ1(R)Θ2(T)=Θ2(R)Θ1(T).

    Definition 2.1. [26] If T is a positive stable matrix in Mj(C), then Γ(T) is defined by

    Γ(T)=0exxTIdx;xTI=exp((TI)logx). (2.2)

    The reciprocal Gamma function denoted by Γ1(η)=1/Γ(η) is an entire function of the complex variable η and for any matrix T in Mj(C), the image of Γ1(η) acting on T, denoted by Γ1(T), is also well defined [26]. Furthermore, if

    T+mIis invertible for all integersmN0, (2.3)

    then Γ(T) is invertible, its inverse coincides with Γ1(T) and one gets the formula

    (T)m=T(T+I)(T+(m1)I)=Γ(T+mI)Γ1(T);mN0. (2.4)

    From (2.4), it easily follows, for a nonzero scalar ε and TMj(C), that

    limε0εm(Tε)m=Tm,limε0εm[(Tε)m]1=[Tm]1mN0. (2.5)

    Also, using (2.4), we have

    (T)k+m=(T)m(T+mI)k=(T)k(T+kI)m. (2.6)

    From [18], we observe that

    (1)k(nk)!I=(n)kn!I=(nI)kn!;0kn. (2.7)

    Recently, authors [23] defined the first Appell matrix hypergeometric functions as follows:

    Definition 2.2. For |z|<1 and |w|<1, we have

    F1(ϕ,ϑ,ωφ;z,w)=s=0r=0(ϕ)s+r(ϑ)s(ω)r[(φ)s+r]1zswrs!r!=s=0(ϕ)s(φ)s[(φ)s]1zss!2F1(ϕ+sI,ωφ+sI;w), (2.8)

    where ϕ,ϑ,ω and φ are commutative matrices in Mj(C) such that φ+nI is invertible for all integer nN0.

    Immediately, one observes the following simple identities ([18,23]):

    F1(ϕ,ϑ,ωφ;z,0)=F2(ϕ,ϑ,ωφ,θ;z,0)=F3(ψ,ϕ,φ,ωφ;z,0)=F4(ϕ,ϑθ,φ;z,0)=2F1(ϕ,ϑφ;z), (2.9)

    and

    F1(ϕ,ϑ,0φ;z,w)=F2(ϕ,ϑ,0φ,θ;z,w)=F3(ϕ,ϑ,ω,0φ;z,w), (2.10)

    where F2,F3 and F4 are matrix versions of the classical Appell hypergeometric functions (see, e.g., [23,24,25]) and 2F1 is matrix version of the classical Gauss hypergeometric function [26] under conditions, ϕ,ϑ,ω,φ and θ are commutative matrices in Mj(C) such that φ+nI and θ+nI are invertible for all integer nN0.

    The confluent Appell matrix functions or Humbert matrix functions [27]

    Φ1(ϕ,ϑφ;z,w)=m,n=0(ϕ)m+n(ϑ)n[(φ)m+n]1m!n!zmwn, (2.11)
    Φ2(ϕ,ϑφ;z,w)=m,n=0(ϕ)m(ϑ)n[(φ)m+n]1m!n!zmwn, (2.12)
    Φ3(ϕφ;z,w)=m,n=0(ϕ)m[(φ)m+n]1m!n!zmwn. (2.13)

    In this section, we define a new matrix-valued Appell-type polynomial in terms of the first Appell hypergeometric matrix function F1 and discuss limit (confluence) formulas as follows:

    Definition 3.1. Let ϕ,θ and φ be positive stable and commuting matrices in Mj(C), such that φ satisfies the condition (2.3). Then, for nN0, the first Appell matrix polynomial Fn is defined by

    Fn[ϕ,θφ;z,w]=(φ)nn!F1(nI,ϕ,θφ;z,w). (3.1)

    where F1 is defined in (2.8).

    Remark 3.1. Note that the polynomial Fn is generalize of the Gauss hypergeometric polynomials (1.2) and a matrix version of the class polynomial [28].

    Remark 3.2. Clearly, using the relations (2.9) and (2.10), we obtain other formulas of the Appell matrix polynomial Fn, for example,

    Fn[ϕ,0φ;z,w]=(φ)nn!F2(nI;ϕ,0φ,θ;z,w), (3.2)

    and

    Fn[ϕ,θφ;z,z]=(φ)nn!2F1(nI;ϕ+θ;φ;z). (3.3)

    Upon using (2.5) with (3.1), the following limit (confluence) formulas can be stated

    limε0n![(φ)n]1Fn[ϕ,1εIφ;z,εw]=Φ1(nI,ϕφ;z,w),
    limε0n![(φ)n]1Fn[1εI,θφ;εz,w]=Φ1(nI,θφ;z,w)

    and

    limε0n![(φ)n]1Fn[ϕε,θεφ;εz,εw]=Φ3(nIφ;z,w).

    From the relation (2.5) and the equations (2.11)–(2.13) with above limit formulas, various confluence formulas can be easily obtained.

    Generating matrix {relations} play an important role in the introduce of matrix-valued polynomials and discuss its properties (see, e.g., [17,22]). In this section, we investigate various generating matrix {relations} for the first Appell matrix polynomials as follows:

    Theorem 4.1. The generating matrix function of Fn[ϕ,θφ;z,w] is as

    n=0(λ)n[(φ)n]1Fn[ϕ,θφ;z,w]tn=(1t)λF1(λI;ϕ,θ;φ;zt1t,wt1t), (4.1)

    where ϕ,θ and φ are positive stable andcommuting matrices in Mj(C) such that φ+nI satisfies the spectral condition (2.3) with λCZ0,|t|<1,|z/(1t)|<1 and |w/(1t)|<1.

    Proof. Assume that the left-hand side of (4.1) is denoted by L. Upon using the series expression of (4.1) with (2.6) and (2.7) to L, we observe that

    L=n=0(λ)nn!p+q0(n)p+q(ϕ)p(θ)q[(φ)p+q]1p!q!zpwqtn=p,q=0(λ)p+q(ϕ)p(θ)q[(φ)p+q]1p!q!(zt)p(wt)qn=0(λ+p+q)nn!tn. (4.2)

    Changing the order of summations in (4.2) and make use of the identity

    n=0(λ+p+q)nn!tn=(1t)(λ+p+q),|t|<1,

    then, with a little simplification and the definition (2.8) we arrive at the right-hand side of (4.1).

    As a consequence of Theorem 4.1, we obtain the following corollaries.

    Corollary 4.1. Let ϕ,θ and φ be positive stable and commutingmatrices in Mj(C) such that φ+nI satisfies the spectral condition (2.3) with |t|<1,|z|<1,|w|<1,|t+w|<1 and |t+z|<1. The followinggenerating matrix function holds true:

    n=0Fn[ϕ,θφ;z,w]tn=(1t)ϕ+θφ(1t+zt)ϕ(1t+wt)θ. (4.3)

    Corollary 4.2. Let ϕ,θ and φ be positive stable and commutingmatrices in Mj(C) such that φ+nI satisfies the spectral condition (2.3). Then we have

    n=0[(φ)n]1Fn[ϕ,θφ;z,w]tn=etΦ2(ϕ,θφ;zt,wt), (4.4)

    where Φ2 is defined in (2.12) with |zt|<1 and |wt|<1.

    Corollary 4.3. Let ϕ,θ and φ be positive stable and commutingmatrices in Mj(C) such that φ+nI satisfies the spectral condition (2.3) with |t|<1 and |z/(1t)|<1, the following generating matrix function holdstrue:

    n=0(λ)n[(φ)n]1Fn[ϕ,θφ;z,z]tn=(1t)λ2F1(λI,ϕ+θ;φ;zt1t). (4.5)

    Theorem 4.2. Let ϕ,θ,ω and φ be positive stable andcommuting matrices in Mj(C) such that φ+nI satisfies the spectral condition (2.3) with |t|<min{1(1+|z|)(1+|η|),1(1+|z|)(1+|η|)},|η|<1,|z|<1 and |w|<1. The following bilineargenerating matrix relation holds true:

    n=02F1(nI,ωφ;η)Fn[ϕ,θφ;z,w]tn=(1t)ω+ϕ+θφ(1t+zt)ϕ(1t+wt)θ(1t+ηt)ω×F1(ω;ϕ,θφ;zηt(1t+zt)(1t+ηt),wηt(1t+ηt)(1t+wt)). (4.6)

    Proof. Let S be the left-hand side of (4.6). Then we have

    S=n=0nk=0(nk)(ω)k[(φ)k]1(η)kFn[ϕ,θφ;z,w]tn=k=0(ω)k[(φ)k]1(ηt)kn=0(n+kk)Fn+k[ϕ,θφ;z,w]tn=(1t)ϕ+θφ(1t+zt)ϕ(1t+wt)θ×k=0(ω)k[(φ)k]1(ηt1t)kFk[ϕ,θφ;z1t+zt,w1t+wt],

    which, in view of (4.1), we obtain the coveted result.

    If w=0 in Theorem 3.1, we have the following result:

    Corollary 4.4. Let ϕ,θ,ω and φ be positive stable andcommuting matrices in Mj(C) such that φ+nI satisfies the spectral condition (2.3) with |t|<min{1(1+|η|),1(1+|z|)},\; |η|<1, and |z|<1. Then we have

    n=0(φ)nn!2F1(nI,ωφ;η) 2F1(nI,ϕφ;z)tn=(1t)ω+ϕφ(1t+zt)ϕ(1t+ηt)ω×2F1(ω,ϕφ;ηzt(1t+zt)(1t+ηt)). (4.7)

    In this section, we consider some recurrence relations for the first Appell matrix polynomial.

    Theorem 5.1. Let Fn[ϕ,θφ;z,w] be given in (3.1), the following recurrence relation holds true:

    zDzFn[ϕ,θφ;z,w]+wDwFn[ϕ,θφ;z,w]nFn[ϕ,θφ;z,w]=(θ+(n1)I)Fn1[ϕ,θφ;z,w],  (5.1)

    where n1 and φ,ϕ and θ are positive stableand commuting matrices in Mj(C) such that φ+nI is invertible for all integer n0, such that Dz=z,Dw=w.

    Proof. To prove (5.1) we consider

    Λ=etΦ2(ϕ,θφ;zt,wt), (5.2)

    where Φ2 is given in (2.12). Then

    DzΛ=tφ1ϕetΦ2(ϕ+I,θφ+I;zt,wt), (5.3)
    DwΛ=tφ1θetϕ2(ϕ,θ+Iφ+I;zt,wt) (5.4)

    and

    DtΛ=etΦ2(ϕ,θφ;zt,wt)zφ1ϕetΦ2(ϕ+I,θφ+I;zt,wt)wφ1θetΦ2(ϕ,θ+Iφ+I;zt,wt), (5.5)

    we eliminate Φ2 from (5.3), (5.4) and (5.5) as follows

    zDzΛ+wDwΛtDtΛ=tΛ. (5.6)

    Since

    Λ=n=0[(φ)n]1Fn[ϕ,θφ;z,w]tn

    and using (5.6), we get

    zn=0[(φ)n]1tnDzFn[ϕ,θφ;z,w]+wn=0[(φ)n]1tnDwFn[ϕ,θφ;z,w]n=0[(φ)n]1nFn[ϕ,θφ;z,w]tn=n=1[(φ)n1]1tnFn1[ϕ,θφ;z,w], (5.7)

    from which it follows that

    zDzFn[ϕ,θφ;z,w]+wDwFn[ϕ,θφ;z,w]nFn[ϕ,θφ;z,w]=(φ+(n1)I)Fn1[ϕ,θφ;z,w]. (5.8)

    This finishes the proof of Theorem 5.1.

    Theorem 5.2. For n1, the recurrence relation for the first Appell matrix polynomials is as

    nFn[ϕ,θφ;z,w]=(φ+2(n1)I)Fn1[ϕ,θφ;z,w]×zϕFn1[ϕ+I,θφ;z,w]wθFn1[ϕ,θ+Iφ;z,w](φ+(n2)I)Fn2[ϕ,θφ;z,w] (5.9)

    where ϕ,θ and φ be positive stable and commuting matrices in Mj(C) such that φ+nI is invertible for all integer nN0.

    Proof. To prove (5.9), assume that

    Q=(1t)φ(1+zt1t)ϕ(1+wt1t)θ. (5.10)

    Then, we get

    (1t)DzQ=tϕ(1t)φ(1+zt1t)(ϕ+I)(1+wt1t)θ, (5.11)

    and

    (1t)DwQ=tθ(1t)φ(1+zt1t)ϕ(1+wt1t)(θ+I), (5.12)

    But

    Q=n=0Fn[ϕ,θφ;z,w]tn, (5.13)

    it follows that

    DzFn[ϕ,θφ;z,w]=DzFn1[ϕ,θφ;z,w]ϕFn1[ϕ,θφ+I;z,w], (5.14)

    and

    DwFn[ϕ,θφ;z,w]=DwFn1[ϕ,θφ;z,w]θFn1[ϕ+I,θφ;z,w]. (5.15)

    Elimination of the derivatives from (5.1), (5.14) and (5.15) leads us to the recurrence relation

    nFn[ϕ,θφ;z,w]=(φ+2(n1)I)Fn1[ϕ,θφ;z,w]×zϕFn1[ϕ+I,θφ;z,w]wθFn1[ϕ,θ+Iφ;z,w](φ+(n2)I)Fn2[ϕ,θφ;z,w]. (5.16)

    This completes the proof of Theorem 5.2.

    Here, we present Rodrigues' type formula of the first Appell matrix polynomial in the following theorem:

    Theorem 6.1. For n,kN0, the following Rodrigues' type formulaholds true:

    Fk[ϕ,θφ;ztzt1,wtwt1]=tIφ(1zt)ϕ(1wt)θn!Dnt[tφ+(n1)I(1zt)ϕ(1wt)θ], (6.1)

    where ϕ,θ and φ be positive stable and commutingmatrices in Mj(C) such that φ+nI is invertible for all integer nN0 with |t|<1,|zt|<1,|wt|<1,|ztzt1|<1 and |wtwt1|<1.

    Proof. From the Binomial matrix formula, see [18]

    m=0(ϕ)mm!um=(1u)ϕ,|u|<1,

    and the definition of first Appell matrix polynomial Fk, see (3.1), we easily have

    Dnt[tφ+(n1)I(1zt)ϕ(1wt)θ]=nr=0(nr)Dnrt[tφ+(n1)I]Drt[(1zt)ϕ(1wt)θ]=nr=0(nr)(rk)(φ)n(ϕ)rk(θ)k[(φ)r]1zrkwk×tφ+(n1)I(1zt)ϕ(rk)I(1wt)(θ+kI)=tφI(1zt)ϕ(1wt)θ×k+sn(n)k+s(φ)n(ϕ)k(θ)s[(φ)k+s]1k!s!(ztzt1)k(wtwt1)s=n!tφI(1zt)ϕ(1wt)θFk[ϕ,θφ;ztzt1,wtwt1].

    The above equation gives the proof of Theorem 6.1.

    In this section, we show certain integral representation for the first Appell matrix polynomial by the product of (3.3) as follows

    Fm[ϕ1,θ1φ1;z,z]Fn[ϕ2,θ2φ2;w,w]=(φ2)n(φ2)mm!n!2F1(mI,ϕ1+θ1φ1;z)2F1(nI,ϕ2+θ2φ2;w)=Γ(φ1+mI)Γ(φ2+nI)mr=0ns=0Γ(m+nrs+1)Γ(mr+1)Γ(ns+1)×Γ(φ1+φ2+(r+s1)I)Γ1(φ1+rI)Γ1(φ2+sI)×1Γ(m+nrs+1)Γ1(φ1+φ2+(r+s1)I)×(1)r+s(ϕ1+θ1)r(ϕ2+θ2)szrwsr!s!. (7.1)

    Changing the order of summations in (7.1) and applying the integral formula

    Γ(A+B+I)Γ1(A+I)Γ1(B+I)=2A+Bππ/2π/2exp((AB)αi)cosA+Bαdα,A,BMj(C),˜μ(A+B)>1,

    then, with a little simplification, we arrive at

    Fm[ϕ1,θ1φ1;z,z]Fn[ϕ2,θ2φ2;w,w]=2φ1+φ2+(m+n2)Iπ2Γ1(φ1+φ2+(m+n1)I)Γ(φ1+mI)Γ(φ2+nI)×π/2π/2π/2π/2exp((φ1φ2)αi+(mn)Iβi)cosφ1+φ22Iαcosm+nβ×Fm+n[ϕ1+θ1,ϕ2+θ2φ1+φ2I;ze(αβ)icosαsecβ,we(αβ)icosαsecβ]dαdβ. (7.2)

    Therefore the following theorem can be investigated.

    Theorem 7.1. Assume that ϕ1,θ1,φ1ϕ2,θ2 and φ2 are positive stable and commutativematrices in Mj(C), such that φ1,φ2 satisfies the condition (2.3) and ˜μ(φ1+φ2)>1. Then, theintegral representation (7.2) holds true.

    Remark 7.1. Note that when j=1, the provided formulas are reduced to those of the classical Appell polynomial F1 (cf. [28]).

    Suppose that

    H=F1(nI,ϕ,θφ;z,w)=n!(φ)nFn[ϕ,θφ;z,w]=ns=0nr=0Us,r(z,w). (8.1)

    Denoting the partial differential operator by

    D=θ1+θ2, (8.2)

    where θ1=zz and θ2=ww. This operator has the particularly pleasant property

    Dzswr=(s+r)zswr.

    Now, the following partial differential equation for the first Appell hypergeometric matrix polynomial of two complex variables can be deduced

    D[ID+φI]H=ns,r=0(s+r)((s+r)I+φI)(nI)s+r(ϕ)s(θ)r[(φ)s+r]1zswrs!r!=ns,r=0(s+r)(nI)s+r(ϕ)s(θ)r[(φ)s+r1]1zswrs!r!=zs,r=0(ϕ+sI)(nI+(s+r)I)Us,r(z,w)+wns,r=0(θ+rI)(nI+(s+r)I)Us,r(z,w)=z(IDnI)(θ1I+ϕ)H+w(IDnI)(θ2I+θ)H.

    We readily see that the first Appell hypergeometric matrix polynomial F1 should be a solution of a partial differential equation given by

    {D[ID+φI](IDnI)[z(θ1I+ϕ)+w(θ2I+θ)]}H=0. (8.3)

    Remark 8.1. Similarly, we can indicate other matrix partial differential equations as special cases of (8.3). For example,

    {IDIzθ1Iwθ2(zϕ+wθ)}F1(nI,ϕ,θnI;z,w)=0.

    The area of matrix polynomial theory has been fast developing and is presently being applied in many fields such as probability theory, physics, scattering theory, statistics, engineering and chemical applications (see, e.g., [17,18,19]). In particular, the 2D special matrix polynomials are very advantageous in several areas of mathematics, prediction theory and spectral analysis. These polynomials allow the derivation of a number of useful identities in a fairly straight forward way and help in introducing new families of special polynomials. For example, Abdalla and Hidan [29] have established the properties of 2D Jacobi matrix polynomials associated with applications. Khan and Raza have proposed many interesting results on two variable Hermite generalized matrix polynomials in [30]. Also, Fuli [31] introduced 2D Shivleys matrix polynomials and studied some its properties. Very recently, results for certain 2D hybrid families related to the Appell matrix polynomials are derived by Nahid and Khan [14,15].

    Motivated by the previous works, In this paper, we introduce the first Appell matrix polynomials of two complex variables and discuss many its properties. It is interesting to note that the matrix polynomials here lead to the generalization of several matrix polynomials into the two variable forms of the hypergeometric, Laguerre, Hermite, Bernoulli, Jacobi, Legendre and truncated exponential matrix polynomials (see, [22]). In addition, this approach allows to derive several new results that can be used in theoretical and applicable aspects and for some numerical algorithm.

    The authors extends their appreciation to the Deanship of Scientific Research at King Khalid University for funding this work through the Research Groups Program [grant number R.G.P.2/11/43].

    The authors declare there is no conflicts of interest.



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