Research article Special Issues

Incomplete exponential type of R-matrix functions and their properties

  • In the present paper, we establish the incomplete exponential type (IEF) of R-matrix functions and identify some properties of the incomplete exponential matrix functions including integral representation, some derivative formula and generating functions of the incomplete exponential of R-matrix functions. Finally, special cases of the presented results are pointed out.

    Citation: Ahmed Bakhet, Mohra Zayed. Incomplete exponential type of R-matrix functions and their properties[J]. AIMS Mathematics, 2023, 8(11): 26081-26095. doi: 10.3934/math.20231329

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  • In the present paper, we establish the incomplete exponential type (IEF) of R-matrix functions and identify some properties of the incomplete exponential matrix functions including integral representation, some derivative formula and generating functions of the incomplete exponential of R-matrix functions. Finally, special cases of the presented results are pointed out.



    The incomplete exponential functions (IEF) introduced by Chaudhry and Qadir [1] considered two classes of functions:

    e[(θ;(x,z))]:=n=0γ(θ+n;x)Γ(θ+n)znn! (1.1)

    and

    E[[θ;(x,z)]]=n=0Γ(θ+n;x)Γ(θ+n)znn!, (1.2)

    such that the incomplete gamma functions γ(θ;x) and Γ(θ;x) defined by Srivastava, Chaudhry and Agarwal [2] as

    γ(θ;x)=x0tθ1etdt (1.3)

    and

    Γ(θ;x)=xtθ1etdt, (1.4)

    respectively, and they achieved the following decomposition:

    γ(θ;x)+Γ(θ;x)=Γ(θ). (1.5)

    The pRq(ϕ,φ;z) function [3] is defined as:

    pRq(ϕ,φ;z)=pRq(θ1,,θpη1,,ηq|ϕ,φ;z)=n01Γ(ϕn+φ)(θ1)n(θp)n(η1)n(ηq)nznn!, (1.6)

    where p,qZ+, ϕ,φC and Re(ϕ),Re(φ),Re(θi),Re(ηj)>0, for i=1,2,,p,j=1,2,,q, and (θ)n denotes the Pochhammer symbol which defined by:

    (θ)n={θ(θ+1)(θ+n1)=Γ(θ+n)Γ(θ),n1,1,n=0. (1.7)

    Exploring the extension of classical matrix functions and matrix polynomials has recently become a prominent topic. Special matrix functions such as Gamma, Beta were studied by Jódar and Cortès who studied matrix analogues of gamma, beta and Gauss hypergeometric functions [4,5,6] and other contributions have been directed to discuss the polynomials in two variables such as the 2-variables Shivley's matrix polynomials [7], the 2-variables Laguerre matrix polynomials [8], the 2-variables Hermite generalized matrix polynomials [9,10,11,12], the 2-variables Gegenbauer matrix polynomials [13] and the second kind of Chebyshev matrix polynomials with two variables [14].

    In the current study, we intend to establish incomplete exponential matrix functions. Involving the pRq(P,Q;z) functions of matrix parameters, we investigate some properties of an incomplete exponential of type of R -matrix functions. Furthermore, we provide generating formulas for the incomplete exponential type of R -matrix functions.

    The paper is organized as follows. In Section 2, we review basic definitions and previous results which will be mandatory through the following sections. Section 3 introduces the definition of the incomplete exponential of type of R -matrix functions and states some theorems about integral and derivative formula of the incomplete exponential of type of R -matrix functions. Some generating matrix relations incomplete exponential of type of R -matrix functions are provided in Section 4. In Section 5, we discuss some special cases of the incomplete exponential of type of R-matrix functions. The paper is appended with conclusions in Section 6.

    Throughout this paper, we consider a matrix L Ch×h and its spectrum σ(L) represents the collection of all eigenvalues L. Let Ch denote the h-dimensional complex vector space and Ch×h denote all square matrices with h rows and h columns with complex entries. As usual, let Re(z) and Im(z) be referring to the real and imaginary parts of a complex number z, respectively. The two-norm of L is defined on Ch×h as follows

    L2=supx0Lx2x2=max{λ:λσ(LL)},xCh, (2.1)

    where for a vector xCh, x2=(xx)12 is the Euclidean norm of x such that L denotes the transposed conjugate of L. Let us denote the real numbers α(L) and β(L) as in the following

    α(L)=max{Re(z):zσ(L)},β(L)=min{Re(z):zσ(L)}. (2.2)

    If f(z) and g(z) are holomorphic functions of the complex variable established in an open set Ω of the complex plane and L, M are matrices in Ch×h with σ(L)Ω and σ(M)Ω, such that LM=ML, then it follows from the matrix functional calculus properties in [7]), that f(L)g(M)=g(M)f(L).

    We recall that the reciprocal Gamma function, given by Γ1(z)=1Γ(z), is an entire function of the complex variable, and thus Γ1(L) is a well defined matrix for any matrix L in Ch×h. In addition, if L is a matrix, then

    L+nIis invertible for all integersn0, (2.3)

    where I is the identity matrix in Ch×h. Then Γ(L) is invertible and its inverse coincides with Γ1(L). The Pochhammer symbol of a matrix argument is given by (see [5]):

    (L)n={L(L+I)(L+(n1)I)=Γ1(L)Γ(L+nI),n1,I,n=0. (2.4)

    Assume that L and M are positive stable matrices in Ch×h. The Gamma matrix function Γ(L) and Beta matrix function B(L,M) have been defined in [5,15], as follows:

    Γ(L)=0ettLIdt,B(L,M)=10tLI(1t)MIdt, (2.5)

    where tLI=exp((LI)lnt). Jódar and Cortés showed in [5] that

    Γ(L)=limn(n1)![(L)n]1nL, (2.6)

    where n1 is an integer.

    Now, the incomplete matrix gamma is defined as follows: [15,16]. Assume that L is a positive stable matrix in Ch×h and y be a positive real number. Then, the incomplete matrix gamma function γ(L,y) and its complement Γ(L,y) are defined by

    γ(L,y)=y0ettLIdt, (2.7)
    Γ(L,y)=yettLIdt, (2.8)

    and we have the following decomposition formula (see [15]):

    γ(L,y)+Γ(L,y)=Γ(L). (2.9)

    The following provides the hypergeometric matrix function 2F1(L,M;N;z) as, assume that L,M and N are matrices in Ch×h and N satisfy condition (2.3), then the hypergeometric matrix function of 2-numerator and 1-denominator for |z|<1 is defined by the matrix power series (see [5,6])

    2F1(L,M;N;z)=n0(L)n(M)n[(N)n]1n!zn. (2.10)

    The Bessel matrix function JL(z) of the first kind associated to L is given in the following form: (see [15,16])

    JL(z)=k=0(1)k(k)!Γ1(L+(k+1)I)(z2)L+2kI (2.11)

    and the modified Bessel matrix function IL(z) has been defined in the form:

    IL(z)=k=01(k)!Γ1(L+(k+1)I)(z2)L+2kI, (2.12)

    where L is a matrix in Ch×h satisfying the condition (2.3). We may rewrite the Bessel and modified Bessel matrix functions as

    JL(z)=(z2)AΓ1(L+I)0F1(;L+I,z24), (2.13)

    and

    IL(z)=(z2)AΓ1(L+I)0F1(;L+I,z24), (2.14)

    where 0F1(;L+I,z24) is a hypergeometric matrix function of 1-denominator

    0F1(;L+I;z24)=n0[(L+I)n]1n!(z24)n.

    Recently, the authors of [17] introduced an extension of the generalized hypergeometric matrix function pRq(P,Q;z) with regard to the matrices occurring in its series representation. Furthermore, they provided integral representations, contiguous matrix function relations, and differential formulas satisfied by the matrix function pRq(P,Q;z) and they used the notation (P) to denote the array of p×p matrices P1,P2,,Pk for some kN.

    For 1ip,1jq, suppose that P,Q,Si and Dj are positive stable matrices in Ch×h such that Dj+kI are invertible for all integers k0, then the matrix function denoted by pRq(P,Q:(S),(D);z) is defined as

    pRq(P,Q:(S),(D);z)=pRq(S1,,SpD1,,Dq|P,Q;z)=n0Γ1(nP+Q)(S1)n(Sp)n×(D1)1n(Dq)1nznn!=pRq[SpDq|P;Q;z], (2.15)

    whenever the series converges absolutely and Sp=S1,,Sp, Dq=D1,,Dq.

    Let L be a matrix in Ch×h. We define the incomplete exponential matrix functions (IEMFs) as follows:

    e[(L;(x,z))]=n=0Γ1(L+nI)γ(L+nI;x)znn! (3.1)

    and

    E[[L;(x,z)]]=n=0Γ1(L+nI)Γ(L+nI;x)znn!, (3.2)

    so that

    e[(L;(x,z))]+E[[L;(x,z)]]=ezI. (3.3)

    Next, some important properties of the IEMF are listed below.

    Lemma 3.1. Let L be a matrix in Ch×h. For the two IEMFs; e[(L;(x,z))] and E[[L;(x,z)]] defined in (3.1) and (3.2), respectively, then the following integral representations hold:

    (i)

    e[(L;(x,z))]=Γ1(L)x0uLIeu(n=0[(L)n]1(uz)nn!)du=Γ1(L)x0uLIeu0F1(,L;zu)du.

    (ii)

    E[(L;(x,z))]=Γ1(L)xuLIeu(n=0[(L)n]1(tz)nn!)dt=Γ1(L)xuLIeu0F1(,L;zt)dt.

    Proof. By replacing the incomplete gamma matrix functions in (3.1) and (3.2), respectively, by their integral representations, we obtain the integral representations of (i) and (ii).

    Lemma 3.2. Let L be a matrix in Ch×h, then the two IEMFs; e[(L;(x,z))] and E[[L;(x,z)]] defined in (3.1) and (3.2), respectively, satisfy the differential properties:

    (i) ze[(L;(x,z))]=n=0Γ1(L+nI)γ(L+nI;x)zn1(n1)!,

    (ii) zE[(L;(x,z))]=n=0Γ1(L+nI)Γ(L+nI;x)zn1(n1)!,

    (iii) ze[(L;(x,z))]=e[(L+I;(x,z))],

    (iv) zE[(L;(x,z))]=E[(L+I;(x,z))].

    Proof. We differentiate (3.1) and (3.2) with respect to z, to conclude (ⅰ) and (ⅱ) respectively. To verify (ⅲ), we replace n by n1 in (ⅰ) and L by L+I, Changing n to n1 in (ⅱ) and L to L+I, immediately imply (ⅳ).

    Remark 3.3. By the integral representation in Lemma 3.2, we define the incomplete matrix exponential by using Bessel matrix function in the form:

    e[(L;(x,z))]=zL2x0tL2etI(L)(22t)dt,E[(L;(x,z))]=zL2xtL2etI(L)(22t)dt,e[(L+I;(x,z))]=zL2x0tL2etJL(22t)dt,

    and

    E[(L+I;(x,z))]=zL2xtL2etJL(22t)dt. (3.4)

    Now, we provide the definition of the incomplete exponential of R-matrix function as

    Definition 3.4. Let L,M,Cp,Dq in Ch×h such that Dq+I satisfying the condition (2.3), then we define the incomplete exponential of R-matrix functions as

    peq[((L,M;x);z)]=peq[CpDq|L,M;x;z]=n=0Γ1(nL+M)γ(nL+M;x)(Cp)n[(Dq)n]1znn! (3.5)

    and

    pEq[(L,M;x;z)]=pEq[CpDq|L,M;x;z]=n=0Γ1(nL+M)Γ(nL+M;x)(Cp)n[(Dq)n]1znn!. (3.6)

    Using (3.5) and (3.6), we obtain the following decomposition formula:

    peq[CpDq|L,M;x;z]+pEq[CpDq|L,M;x;z]=pFq[CpDq|z], (3.7)

    where pFq(.) is the generalized hypergeometric matrix function defined in [18].

    Remark 3.5. For p=0,q=0,L=I, the expressions (3.5) and (3.6) reduce to the incomplete exponential matrix functions in (3.1) and (3.2) as

    peq[(I,M;x;z)]=0e0[CpDq|I,M;x;z]=n=0Γ1(nI+M)γ(nI+M;x)znn!=e[((M,x);z)] (3.8)

    and

    0E0[(I,M;x;z)]=0E0[CpDq|I,M;x;z]=n=0Γ1(nI+B)Γ(nI+M;x)znn!=E[(M,x;z)]. (3.9)

    In the current section, we deduce several integral representations of the incomplete exponential of R-matrix functions.

    Theorem 3.6. The incomplete exponential of R-matrix function pEq[(L,M;x;z)] matrix function satisfies the following integral representations:

    pEq[(L,M;x;z)]=pEq[CpDq|L,M;x;z]=xtMIetpRq[CpDq|L,M;ztL]dt, (3.10)

    where L,M,Cp and Dq are commuting matrices in Ch×h, β(M)>0,β(nL+M)>0,β(Cp)>0 and Dp+I satisfies the condition (2.3).

    Proof. By using the definition of complement of gamma matrix function defined by (2.8), we obtain

    pEq[CpDq|L,M;x;z]=xtnL+MIet[n=0Γ1(nL+M)(Cp)n[(Dq)n]1znn!]dt. (3.11)

    By reversing the order of summation and integration and using Lemma 6 in [19], we find

    pEq[CpDq|L,M;x;z]=xtMIet[n=0Γ1(nL+M)(Cp)n[(Dq)n]1(ztL)nn!]dt,

    and this completes the proof of Theorem 3.6.

    From the proof of the previous Theorem 3.6, we conclude the following result.

    Corollary 3.7.

    (i) By setting L=I, M=C and p=1,q=0, then, C1=A in (3.11) and noting that all matrices are commutative, we get

    1E0[A|I,C;x;z]=Γ1(C)x[uCIeu1F1[AC|zu]]du, (3.12)

    where 1F1 is hypergeometric matrix function in (2.10)

    (ii) From R-matrix function, we have the integral matrix representation as

    pRq[CpDq|L,M;z]=Γ1(C1)0[uC1Ieup1Rq[Cp1Cq|L,M;uz]]du, (3.13)

    where pq+1.

    Theorem 3.8. Let L,M,Cp and Dq be commuting matrices in Ch×h, β(M)>0,β(nL+M)>0,β(Cp)>0 and Dq+I satisfying the condition (2.3), then the incomplete exponential of R-matrix function pEq[(L,M;x;z)] matrix function have the following integral representation:

    pEq[CpDq|L,M;x,z]=Γ1(C1)Γ1(D1C1)Γ(D1)10[tC1I(1t)D1C1Ip1Eq1[Cp1Cq1|L,M;x,zt]]dt. (3.14)

    Proof. By using integral definition of Beta matrix function

    (M)n[(C)n]1=Γ1(M)Γ1(CM)Γ(C)10tM+(n1)I(1u)CBMIdt. (3.15)

    By substituting (3.15) in (3.14), it follows that

    pEq[CpDq|L,M;x,z]=n=0Γ1(nL+M)Γ(nL+M;x)(Cp)n[(Dq)n]1znn!=Γ1(C1)Γ1(D1C1)Γ(D1)n=0Γ1(nL+M)Γ(nL+M;x)(Cp1)n[(Dq1)n]1znn!10tC1+(n1)I(1u)D1C1Idt. (3.16)

    Further simplification and reversing the order and integration leads to the required result.

    Theorem 3.9. For R-matrix function the incomplete exponential have the following derivative formula.

    dndzn{pEq[CpDq|L,M;x,z]}=(Cp)n[(Dq)n]1pEq[Cp+nIDq+nI|L,L+M;x,z], (3.17)

    where L,M,Cp,Dq are commuting matrices Ch×h.

    Proof. From Eq (3.6) by differentiating with respect to z and replacing n by n+1, we get

    ddz{pEq[CpDq|;L,M;x,z]}=n=0Γ1(L(n+1)+M)Γ(L(n+1)+M;x)(Cp)n+1[(Dq)n+1]1znn!, (3.18)

    using the relation (L)n+1=L(L+I)n, we find that

    ddz{pEq[CpDq|;L,BM;x,z]}=(Cp)[(Dq)]1pEq[Cp+IDq+I|L,L+M;x,z]. (3.19)

    By repeating above procedure n-times yields the R.H.S. of assertion (3.17).

    Theorem 3.10. Suppose that L,M,Cp and Dq are commuting matrices in Ch×h and Dq+I satisfying the condition (2.3), then, the incomplete exponential of R-matrix function pEq[(L,M;x;z)] matrix function have the following partial derivatives holds true:

    z{pEq[CpDq|;L,M;x,z]}=(Cp)n[(Dq)n]1pEq[Cp+IDq+I|L,L+M;x,z] (3.20)

    and

    z{pEq[CpDq|;L,M;x,z]}=exxBIpEq[Cp+IDq+I|L,L+M;x,zxA]. (3.21)

    Proof. Differentiating partially (3.6) with respect to z, it follows that:

    z{pEq[CpDq|;L,M;x,z]}=z{n=0Γ1(nL+M)Γ(nL+M;x)(Cp)n[(Dq)n]1znn!}=n=0Γ1(nL+M)Γ(nL+M;x)(Cp)n[(Dq)n]1zn1(n1)!. (3.22)

    By replacing n by n+1 in the Eq (3.21). For the proof (3.22), By using differentiate partially first integral representation (3.11) with respect to x.

    This section is devoted to exploring some generating functions of the incomplete exponential of R-matrix functions. Furthermore, several linear generating relations of the R-matrix function of the incomplete exponential function is deduced.

    Theorem 4.1. Let L,M,Cp, and Dq are commuting matrices in Ch×h such that Dj+kI,1<j<q are inevitable for all integers k0. Then, the generating function of the incomplete exponential of R-matrix functions is given as:

    u0tLI(ut)MIpEq[CpDq|;L,M;x,λtk]dt=B(L,M)uL+MIp+kEq+k[Cp,Δ(k,L)Dq,Δ(k,L+M)|;L,M;x,λuk], (4.1)

    where k is a positive integer and Δ(k,L) represents the sequence matrix of k parameters as

    Lk,L+Ik,L+2Ik,,L+(k1)Ik.

    Proof. Let w1 be the left hand side of Eq (4.1). Then, by using (3.6), this gives

    w1=u0tLI(ut)MIn=0Γ1(nL+M)Γ(nL+M;x)×(Cp)n[(Dq)n]1(λtk)nn!dt. (4.2)

    By substituting t=ux, we have

    w1=uL+MI10xL+(kn1)I(1t)MIΓ1(nL+M)Γ(nL+M;x)(Cp)n[(Dq)n]1(λtk)nn!dx=uL+MIn=0Γ1(nL+M)Γ(nL+M;x)×(Cp)n[(Dq)n]1Γ1(L+M+knI)Γ(L+knI)Γ(M)(λtk)nn!. (4.3)

    Therefore, using the property Pochhammer matrix symbol leads directly to the right hand side of Eq (4.1).

    Theorem 4.2. Let L,M,Cp, and Dq are commuting matrices in Ch×h such that Dj+kI,1<j<q are inevitable for all integers k0. A linear generating relation for the R-matrix function of incomplete exponential can be given as:

    xt(xu)EI(ut)MIpEq[CpDq|;L,M;x,λ(ut)k]du=Γ(E)Γ(M)Γ1(M+E)(xt)E+MIp+kEq+k[Cp,Δ(k,L)Dq,Δ(k,E+M)|;L,M;x,λ(xt)k]. (4.4)

    Proof. Let w2 be the left hand side of Eq (4.4) and by using (3.6), we obtain

    w2=Γ1(M)Γ1(E)Γ(M+E)xt(xu)EI(ut)MIn=0Γ1(nL+M)Γ(nL+M;x)(Cp)n[(Dq)n]1(λ(ut)k)nn!dt. (4.5)

    Now, by substituting m=utxt, it follows that

    w2=Γ1(M)Γ1(E)Γ(M+E)(xt)E+MI10mM+(kn1)I(1m)EIn=0Γ1(nL+M)Γ(nL+M;x)(Cp)n[(Dq)n]1(λ(xt)k)nn!dm=Γ1(M)Γ1(E)Γ(M+E)(xt)E+MIn=0Γ1(nL+M)Γ(nL+M;x)Γ1(E+M+knI)Γ(M+knI)Γ(E)(Cp)n[(Dq)n]1(λ(xt)k)nn!. (4.6)

    Thus, using the properties of Pochhammer matrix implies the right-hand side of (4.4).

    Now, we provide some linear generating relations for the R-matrix function of generalized incomplete exponential as follows.

    Theorem 4.3. Let L,M,Cp, and Dq are commuting matrices in Ch×h such that Dj+kI,1<j<q are inevitable for all integers k0. Then, the following linear generating relation for the R-matrix function of incomplete exponential hold:

    n=0[(k1)IEk]peq+1[CpDq,E(k1)I|;L,M;x,z]tk=(1t)Epeq+1[CpDq,IE|;L,M;x,z(1t)], (4.7)

    where |z|<1.

    Proof. Let w3 be the left-hand side of (4.7) and by applying (3.5), we obtain that

    w3=k=0[(k1)IEk](n=0Γ1(nL+M)Γ(nL+M;x)[(E(k1)I)n]1(Cp)n[(Dq)n]1znn!)tk. (4.8)

    By reversing the order of summation and using the relation

    (E(k1)I)n=(E+I)n[(k1)IEk].[(kn1)IEk]1k,nN, (4.9)

    where

    (Ek)=Γ1(k+1)Γ1(E(k1)I))Γ(E+I), (4.10)

    we obtain

    w3=n=0Γ1(nL+M)Γ(nL+M;x)[(Ek)n]1(Cp)n[(Dq)n]1znn!k=0[(kn1)IEk]tk. (4.11)

    Moreover, we find the inner sum in (4.11), by using the relation

    k=0[(k1)IEk]tk=(1t)E. (4.12)

    From (4.11) and (4.12), the right hand side of (4.7) yields.

    Theorem 4.4. Let L,M,Cp, and Dq are commuting matrices in Ch×h such that Dj+kI,1<j<q are inevitable for all integers k0. Then

    k=0[(k1)IEk]pEq+1[CpDq,E(k1)I|;L,M;x,z]tk=(1t)EpEq+1[CpDq,IE|;L,M;x,z(1t)], (4.13)

    where |z|<1.

    Proof. The proof here runs similarly to the the proof of Theorem 4.3. The details are omitted.

    Remark 4.5. If we add the generating Eqs (4.7), (4.13) and using (3.7), then we have the following generating form as

    k=0[(k1)IEk]pFq+1[CpDq,E(k1)I|z]tk=(1t)EpFq+1[CpDq,E(k1)I|z(1t)]. (4.14)

    In this section, we discuss some special cases of generalized incomplete exponential matrix functions as stated in the following theorems:

    Theorem 5.1. Let L,M,Cp, and Dq are commuting matrices in Ch×h such that Dj+kI,1<j<q are inevitable for all integers k0. Then

    2E1[C1,C2D1|L,M;x;1]=Γ1(D1C1)Γ1(D1C2)Γ(D1)Γ(D1C1C2)γ(nL+M;x)2R1[|L,M;z]. (5.1)

    Proof. Putting z=1,p=2,q=1 in the decomposition formula (3.7) implies that

    2E1[C1,C2D1|L,M;x;1]=2F1[C1,C2D1|1]2e1[C1,C2D1|L,M;x,z]=2F1[C1,C2D1|1]x0tMIet2R1[C1,C2D1|L,M;ztL]dt=2F1[C1,C2D1|1]x0tMIetn=0Γ1(nL+M)[(D1)n]1x(C1)n(C2)n(ztL)nn!dt. (5.2)

    By using the relation of Gauss matrix summation [18] and reversing the order of summation and integration, we find that

    2E1[C1,C2D1|L,M;x;1]=Γ1(D1C1)Γ1(D1C2)Γ(D1)Γ(D1C1C2)n=0Γ1(nL+M)[(D1)n]1(C1)n(C2)nznn!x0tnL+M1etdt. (5.3)

    Further simplification leads to the right-hand side of (5.1).

    Theorem 5.2. Let L,M,Cp, and Dq be commuting matrices in Ch×h such that Dj+kI,1<j<q are inevitable for all integers k0. Then

    (C1D1+I)2E1[C1,C2D1|L,M;x;z]=2E1[C1+I,C2D1|L,M;x;z](D1I)2E1[C1,C2D1I|L,M;x;z]. (5.4)

    Proof. Let w4 be the L.H.S of (5.4), then by using (3.6), we find that

    w4=n=0Γ1(nL+M)Γ[nL+M;x][(D1)n]1C1(C1+I)n(C2)n(D1I)[(D1I)n]1znn!. (5.5)

    Employing the relation of Pochhammer matrix implies that

    C1(C1+I)n=(C1+nI)(C1)n

    and

    (D1I)(D1)n=(D1I)n(D1+(n1)I).

    This yields the left side of (5.4).

    The incomplete exponential type of R-matrix function is exhibited in the current study. Several characterizations of the proposed incomplete exponential pRq(P,Q;z) matrix functions such that the integral representation, the derivative formulas and generating functions of the incomplete exponential of R-matrix functions. We conclude our study by presenting special cases of the obtained results. The findings of the present paper can be extended to obtain some interesting new results by fitting some suitable parameters.

    The authors declare they have not used Artificial Intelligence (AI) tools in the creation of this article.

    The authors extend their appreciation to the Deanship of Scientific Research at King Khalid University for funding this work through large group Research Project under grant number RGP2/310/44.

    The authors declare there is no conflicts of interest.



    [1] M. A. Chaudhry, A. Qadir, Incomplete exponential and hypergeometric functions with applications to the non central χ2 -distribution, Commun. Stat. Theor. M., 34 (2005), 525–535. https://doi.org/10.1081/STA-200052154 doi: 10.1081/STA-200052154
    [2] H. M. Srivastava, M. A. Chaudhry, R. P. Agarwal, The incomplete Pochhammer symbols and their applications tohypergeometric and related functions, Integr. Trans. Spec. Funct., 23 (2012), 659–683. https://doi.org/10.1080/10652469.2011.623350 doi: 10.1080/10652469.2011.623350
    [3] R. Desai, A. K. Shukla, Some results on function pRq(α,β;z), J. Math. Anal. Appl., 448 (2017), 187–197. https://doi.org/10.1016/j.jmaa.2016.10.048 doi: 10.1016/j.jmaa.2016.10.048
    [4] L. Jódar, J. C. Cortés, Some properties of Gamma and Beta matrix functions, Appl. Math. Lett., 11 (1998), 89–93. https://doi.org/10.1016/S0893-9659(97)00139-0 doi: 10.1016/S0893-9659(97)00139-0
    [5] L. Jódar, J. C. Cortés, On the hypergeometric matrix function, J. Comput. Appl. Math., 99 (1998), 205–217. https://doi.org/10.1016/S0377-0427(98)00158-7 doi: 10.1016/S0377-0427(98)00158-7
    [6] L. Jódar, J. C. Cortés, Closed form general solution of the hypergeometric matrix differential equation, Math. Comput. Model., 32 (2000), 1017–1028. https://doi.org/10.1016/S0895-7177(00)00187-4 doi: 10.1016/S0895-7177(00)00187-4
    [7] F. He, A. Bakhet, M. Hidan, M. Abdalla, Two variables Shivley's matrix polynomials, Symmetry, 11 (2019), 151. https://doi.org/10.3390/sym11020151 doi: 10.3390/sym11020151
    [8] S. Khan, N. A. M. Hassan, 2-variables Laguerre matrix polynomials and Lie-algebraic techniques, J. Phys. A Math. Theor., 43 (2010), 235204. https://doi.org/10.1088/1751-8113/43/23/235204 doi: 10.1088/1751-8113/43/23/235204
    [9] R. S. Batahan, A new extension of Hermite matrix polynomials and its applications, Linear Algebra Appl., 419 (2006), 82–92. https://doi.org/10.1016/j.laa.2006.04.006 doi: 10.1016/j.laa.2006.04.006
    [10] H. M. Srivastava, W. A. Khan, H. Haroon, Some expansions for a class of generalized Humbert matrix polynomials, RACSAM, 113 (2019), 3619–3634. https://doi.org/10.1007/s13398-019-00720-6 doi: 10.1007/s13398-019-00720-6
    [11] S. Khan, N. Raza, 2-variable generalized Hermite matrix polynomials and Lie algebra representation, Rep. Math. Phys., 66 (2010), 159–174. https://doi.org/10.1016/S0034-4877(10)00024-8 doi: 10.1016/S0034-4877(10)00024-8
    [12] S. Khan, A. Al-Gonah, Multi-variable Hermite matrix polynomials: Properties and applications, J. Math. Anal. Appl., 412 (2014), 222–235. https://doi.org/10.1016/j.jmaa.2013.10.037 doi: 10.1016/j.jmaa.2013.10.037
    [13] G. S. Kahmmash, A study of a two variables Gegenbauer matrix polynomials and second order matrix partial differential equations, Int. J. Math. Anal., 2 (2008), 807–821.
    [14] L. Kargin, V. Kurt, Chebyshev-type matrix polynomials and integral transforms, Hacet. J. Math. Stat., 44 (2015), 341–350. https://doi.org/10.15672/HJMS.2015449102 doi: 10.15672/HJMS.2015449102
    [15] J. Sastre, L. Jódar, Asymptotics of the modified Bessel and incomplete gamma matrix functions, Appl. Math. Lett., 16 (2003), 815–820. https://doi.org/10.1016/S0893-9659(03)90001-2 doi: 10.1016/S0893-9659(03)90001-2
    [16] L. Jódar, R. Company, E. Navarro, Solving explicitly the Bessel matrix differential equation, without increasing problem dimension, Congr. Numer., 92 (1993), 261–276.
    [17] R. Dwivedi, R. Sanjhira, On the matrix function pRq(A,B;z) and its fractional calculus properties, Commun. Math., 31 (2023), 43–56. https://doi.org/10.46298/cm.10205 doi: 10.46298/cm.10205
    [18] A. Bakhet, F. He, On the matrix version of extended Struve function and its application on fractional calculus, Filomat, 36 (2022), 3381–3392. https://doi.org/10.2298/FIL2210381B doi: 10.2298/FIL2210381B
    [19] T. Cuchta, D. Growb, N. Wintz, Discrete matrix hypergeometric functions, J. Math. Anal. Appl., 518 (2023), 126716. https://doi.org/10.1016/j.jmaa.2022.126716 doi: 10.1016/j.jmaa.2022.126716
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