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Bulletin of Mathematical Analysis and Applications ISSN: 1821-1291, URL: http://www.bmathaa.org Volume 8 Issue 4(2016), Pages 98-111.

ON THE HYPERGEOMETRIC MATRIX k-FUNCTIONS

G. RAHMAN, A. GHAFFAR, S. D. PUROHIT, S. MUBEEN, M. ARSHAD

Abstract. The hypergeometric functions with the matrix arguments are con-sidered to be important as they have many applications described by a number of researchers. In this present paper, we deal with the study of the hypergeo-metrick-functions i.e.,Fk(P, Q;R;z) with the matrix argumentsP,QandR and these matrix arguments satisfy the matrix differential equation in terms of the new parameterk >0 which is the improved version of generalization of classical hypergeometric matrix functions. Further, we obtain an integral representation ofFk(P, Q;R;z) for the case whereQ,RandR−Qare positive stable matrices with the property thatQR=RQby using the definitions of gamma and beta matrixk-functions recently defined by the researchers.

1. Introduction

Most of the special functions encountered in physics, engineering, analytic func-tions and probability theory are special cases of hypergeometric funcfunc-tions ([12, 19],[26]-[29]). A function of matrix argument is a real or complex valued func-tion of the elements of a matrix. Special matrix funcfunc-tions appear in the literature related to Statistics [1], Lie groups theory [11], and more recently in connection with matrix analogues of Laguerre matrix polynomial and system of second or-der differential equations for matrix arguments, orthogonal matrix polynomial and second order differential equations, Hermite and Legendre differential equations and the corresponding polynomial families (see [13]-[16]). Also, many researchers ([8]-[10],[17, 18]) have defined matrix computation, Bessel function of matrix ar-guments, ordinary differential equation of matrix arar-guments, properties of gamma and beta matrices and hypergeometric matrix arguments. Apart from the close relationship with the well-known beta and gamma matrix k-functions, the emerg-ing theory of orthogonal matrix polynomials ([4]-[6]) and its operational calculus suggest the study of hypergeometric matrixk-functions.

The paper is organized as follows: In section 2, we deal with the study of new properties of the beta and gamma matrix k-functions. We are mainly concerned

2000Mathematics Subject Classification. 33B15, 33C15, 33B20, 33C05.

Key words and phrases. Gamma matrixk-function, beta matrixk-function, hypergeometric matrixk-function.

c

2016 Universiteti i Prishtin¨es, Prishtin¨e, Kosov¨e. Submitted May 30, 2016. Published December 22, 2016. Communicated by Huseyin Bor.

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with the matrix analog of the formula

Bk(P, Q) =Γk(P)Γk(Q)

Γk(P+Q) (1.1)

and may be regarded as a continuation of [25]. In Section 3, the Gauss hyperge-ometric matrix k-functions Fk(P, Q;R;z) is introduced as a matrix power series. Conditions for the convergence on the boundary of the unit disc are treated. In section 4, we define some results of an integral representations of hypergeometric matrix k-functions. Recently the researchers have worked on special k-functions (see [20]-[22],[24]). Mubeen et al. [23] defined the solution of hypergeometric k-differential equations. In this paper, we also prove that if matricesQand R com-mutes and are positive stables (where positive stable means if every eigenvalue of the matrix has positive real part), thenFk(P, Q;R;z) is a solution of the differential equation

kz(1−kz)ω00−kzP ω0+ (R−(Q+kI)kz)ω0−P Qω= 0.

IfP is an arbitrary matrix inCr×randRis an invertible matrix whose eigenvalues are not negative integers then we prove that equation

kz(1−kz)ω00−kzP ω0+ (R+ (n−k)kIz)ω0−nP ω= 0 has matrix polynomial solutions of degreenfor all integern≥1.

Finally in Section 4, we define an integral representation of the hypergeometric matrix k-functions. Throughout in this paper, for a matrix P in Cr×r and its spectrumσ(P) denotes the set of all the eigenvalues ofP. The 2-norm ofP will be denoted bykP kand it is defined by

kP k= sup x6=0

kP xk2

kxk2

(1.2)

where for ay inCr×r,kY k2= (yT y)

1

2 is the Euclidean norm of y. Let us denote

σ(P) andβ(P) the real numbers

α(P) = max{Re(z) :z∈σ(P)}, β(Q) = min{Re(z) :z∈σ(P)}. (1.3) Letf(z) andg(z) be two holomorphic functions of the complex variablez, which are defined in an open set Ω of the complex plane, andP is a matrix inCr×rwith σ(P) ⊂ Ω, then from the properties of matrix functional calculus ([3],p.558), it follows that

f(P)g(Q) =g(Q)f(P). (1.4) The reciprocal of gammak-function denoted by Γ−1k = 1

Γk is an entire function of the complex variable. Like wise the image of the inverse gamma matrixk-function acting on the matrix P, denoted by Γ−1k (P) is a well defined matrix for k > 0. Now, if

P+nkI is invertible matrix for every integern≥0 andk >0,

then Γk is invertible and its inverse coincides with Γ−1k (P), and recently Mubeen et al. [25] defined

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In the same paper, they introduced by using the condition thatP+nkIis invertible matrix, then equation (1.5) can be written as

P(P+kI)(P+ 2kI)· · ·(P+ (n−1)kI) = Γk(P+nkI)Γ−1k (P), n≥1, k >0,(1.6) and like the Pochhammerk-symbol for any matrixP inCr×r by application of the matrix functional calculus, they defined

(P)n,k=P(P+kI)(P+ 2kI)· · ·(P+ (n−1)kI), n >0, (P)0=I. (1.7)

The Schur deposition of a matrixP is given by (see [8], pp. 192-193)

ketPk ≤etα(P) r−1 X

i=0

(kPkr12t)

i! , t≥0 (1.8)

2. On Gamma, Beta Matrix k-Functions

In this section, we used the property of commutativity of matrices and extend the matrix framework of gamma and beta k-functions which will be used in section 4 to obtain an integral representation of the hypergeometric matrix k-function. Further more for the sake of clarity in the presentation, we recall the following results recently defined in [25].

Definition 1. Gamma Matrix k-Function [25]. IfP is a positive stable matrix inCr×r,n≥1 is an integer andk >0, then

Γk(P) = lim n→∞n!k

n

(P)−1n,k(nk)Pk−I. (2.1)

Definition 2. Beta Matrix k-Function [25]. IfP andQ are positive stable matrices inCr×r, then betak-function is defined by

βk(P, Q) = 1 k

1 Z

0

tPk−I(1−t) Q

k−Idt. (2.2)

Hence the authors defined that ifP andQare commuting positive stable matrices then βk(P, Q) = βk(Q, P), and commutativity is a necessary condition for the symmetry of betak-function, see [25].

Lemma 2.1. Let P andQ be positive matrices inCr×r such that P Q=QP and satisfy the condition P+Q+mkI is invertible for all integerm≥0 andk >0.

If n≥0is an integer, then the following identities hold: (i)

βk(P, Q+nkI) = (P+Q)−1n,k(Q)n,kβk(P, Q), (ii)

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Proof. (i) Forn= 0 the proof is obvious. Let us assume that 0< m≥nand using the fact thatP Q=QP, it follows that

βk(P, Q+mkI) = 1 k

1 Z

0

tPk−I(1−t) Q

k+(m−1)Idt

= 1 kδlim→0

1−δ

Z

δ

tPk−I(1t) Q

k+(m−1)Idt

= 1 kδlim→0

1−δ

Z

δ

tP+kQ+(m−2)I(1−t) Q

k+(m−1)It−( Q

k+(m−1)I)dt

= 1 kδlim→0

1−δ

Z

δ

u(t)v(t)dt, (2.3)

where

u(t) = (1−t)Qk+(m−1)It−( Q

k+(m−1)I)t P

k, v(t) =t P+Q

k +(m−2)I.

Integrating equation (2.3) by parts, we get βk(P, Q+mkI) = lim

δ→0[k(P+Q+ (m−1)kI)

−1(1t)Q

k+(m−1)ItPk]t=1−δ t=δ

+ lim

δ→0k(P+Q+ (m−1)kI) −1

×

1−δ

Z

δ

{1

k(Q+ (m−1)kI)(1−t) Q

k+(m−2)It P k

+ 1

k(Q+ (m−1)kI)(1−t) Q

k+(m−1)tPk}dt

= k(P+Q+ (m−1)kI)−1(Q+ (m−1)kI)

× 1

k

1 Z

0

(1−t)Qk+(m−1)t P kdt

= (P+Q+ (m−1)kI)−1(Q+ (m−1)kI)

× βk(P, Q+ (m−1)kI). Hence by using an induction, we obtain

βk(P, Q+nkI) = (P+Q)−1n,k(Q)n,kβk(P, Q).

(ii). To prove (ii), we apply (i) by taking ˆP =P+nkI where n≥1. Then by (i) it follows that

βk( ˆP , Q+nkI) = ( ˆP+Q)−1n,k(Q)n,kβk( ˆP , Q). (2.4) SinceP Q=QP, therefore we have ˆP Q=QPˆ andβk( ˆP , Q) =βk(Q,Pˆ). By (2.4) it follows that

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Also by (i), we have

βk(Q, P +nkI) = (Q+P)−1n,k(P)n,kβk(Q, P) = (Q+P)−1n,k(P)n,kβk(P, Q). (2.6) By equations (2.4) and (2.5), we get

βk(P+nkI, Q+nkI) =βk( ˆP , Q+nkI) = (P+Q+nkI)−1n,k(Q)n,k(P)n,k(2.7)

× (Q+P)−1n,kβk(P, Q). (2.8) Now by definition, we have (P+Q+nkI)n,k(Q+P)n,k= (P+Q)2n,k. Hence by substituting in equation (2.7), we get the required result as

βk(P+nkI, Q+nkI) = (P+Q)−12n,k(P)n,k(Q)n,kβk(P, Q).

Lemma 2.2. Let P and Q be commuting matrices in Cr×r such that P, Q and P+Qare positive stable matrices, then

βk(P, Q) = Γk(P)Γk(Q)Γ−1k (P+Q).

Proof. Since the matricesP andQare stable and alsoP Q=QP, we can write it as

Γk(P)Γk(Q) = (

∞ Z

0

uP−Ie−ukk du)(

∞ Z

0

vQ−Ie−vkkdv). (2.9)

By changing of variablesx=uku+kvk andy=u

k+vk, then equation (2.9) becomes

Γk(P)Γk(Q) =

∞ Z

0 1 Z

0

(xy)1k(P−I)e−1k(xy)1 kx

1

k−Iy1k(y(1x))1k(Q−I)e−1k(y(1−x))

× 1

ky

1

k−I(1x)k1dxdy

= (1 k

∞ Z

0

(y)1k(P+Q)−Ie− y kdy)(1

k

1 Z

0

xPk−I(1x) Q

k−Idx). (2.10)

Now by replacingy=tk in the first integral of (2.10), we get

Γk(P)Γk(Q) = (

∞ Z

0

tP+Q−Ie−tkkdt)(1 k

1 Z

0

xPk−I(1x) Q k−Idx)

= Γk(P+Q)βk(P, Q).

Definition 3. Let us consider P and Q be two commuting matrices in Cr×r such that for all integern≥0 and satisfy the condition

P+nkI, Q+nkI, P+Q+nkI ∀ k >0, (2.11) are invertible matrices.

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where [|α(P, Q)|] denotes the entire part function. Then betak-functionβk(P, Q) is defined by

βk(P, Q) = (P)−1n0,k(Q)

−1

n0,k(P+Q)2n0,kβk(P+n0kI, Q+n0kI). (2.12) Theorem 2.3. Let P and Q be two commuting matrices in Cr×r satisfying the condition (2.11) for all integern≥0. then

βk(P, Q) = Γk(P)Γk(Q)Γ−1k (P+Q).

Proof. Suppose thatn0=n0(P, Q) be defined in definition 3, then we can write

βk(P, Q) = (P)−1n0,k(Q)

−1

n0,k(P+Q)2n0,kβk(P+n0kI, Q+n0kI),

whereP+nkI andQ+nkI are positive stable matrices. By (2.4) we can write Γk(P) = Γk(P+n0kI)(P+ (n0−1)kI)−1· · ·(P+kI)−1P−1

= Γk(P+n0kI)(P)−1n0,k,

Γk(Q) = Γk(Q+n0kI)(Q)−1n0,k

and

Γk(P+Q) = Γk(P+Q+ 2n0kI)(P+Q)−12n0,k.

SinceP Q=QP, we can write

Γk(P)Γk(Q)Γ−1k (P+Q)

= Γk(P+n0kI)Γk(Q+n0kI)Γ−1k (P+Q+ 2n0kI)(P)−1n0,k(Q)

−1

n0,k(P+Q)2n0,k.

(2.13) Since we know that the matricesP+n0kI,Q+n0kIandP+Q+ 2n0kIare positive

stable, so by Lemma 2 we get

Γk(P +n0kI)Γk(Q+n0kI)Γ−1k (P+Q+ 2n0kI) = βk(P+n0kI, Q+n0kI),

(2.14) and by Lemma 2.1 (ii), we have

βk(P+n0kI, Q+n0kI) = (P)n0,k(Q)n0,k(P+Q)

−1

2n0,kβk(P, Q). (2.15)

Hence by (2.13)-(2.15), it follows that

βk(P, Q) = Γk(P)Γk(Q)Γ−1k (P+Q).

3. On the Hypergeometric Matrix k-Functions

In this section, we define the hypergeometric matrixk-function which is denoted byFk(P, Q;R;z) wherek >0 and defined as

Fk(P, Q;R;z) =

∞ X

n=0

(P)n,k(Q)n,k(R)−1n,k

n! z

n, (3.1)

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Theorem 3.1. Let P,QandR be positive stable matrices inCr×r such that

β(R)> α(P) +α(Q). (3.2)

Then the series (3.1) is absolutely convergent for |z|= 1.

Proof. Assume that there exist a positive numberδ, then by hypothesis (3.2) we have

β(R)−α(P)−α(Q) = 2δ. (3.3)

Now let us write

(nk)1+δk[1

n!(P)n,k(Q)n,k(R)

−1 n,k] = (nk) 1+δ k n!

(n−1)!kn−1(nk)P

k(nk)−Pk(P)n,k (n−1)!kn−1

× (n−1)!k

n−1(nk)Q k(nk)−

Q k(Q)n,k (n−1)!kn−1 (R)

−1

n,k(nk) R k(nk)−

R k = (nk) 1+δ k n (

(nk)−Pk(P)n,k (n−1)!kn−1 )(nk)

P

kkn−1((nk)

−Q k(Q)n,k (n−1)!kn−1 )(nk)

Q k

× kn−1(n−1)!(R)−1n,k(nk)Rk(nk)− R k

or

(nk)1+δk[1

n!(P)n,k(Q)n,k(R)

−1

n,k]

=kn(nk)δk((nk)

−P k(P)n,k (n−1)!kn−1 )(nk)

P k((nk)

−Q k(Q)n,k (n−1)!kn−1 )

×(nk)Qk((n−1)!kn−1(R)−1 n,k(nk)

R k)(nk)−

R

k. (3.4) By (1.8), we are taking into account thatα(−R) =−β(R) thus we can write

k(nk)Pkk k(nk) Q

kk k(nk)− R

kk ≤ (nk)

1

k(α(P)+α(Q)−β(R)){ r−1 X

j=0

(kPkr12lnn)j

kj! }

× {

r−1 X

j=0

(kQkr12 lnn)j

kj! }{ r−1 X

j=0

(kRkr12 lnn)j

kj! }.

By (3.3), we obtain

k(nk)Pkk k(nk) Q

kk k(nk)− R

kk ≤(nk)−

2δ k{

r−1 X

j=0

[max{kPk,kQk,kRk}r12]j

kj! (lnn)

j}3.

(3.5) Thus with the aid of (3.3)-(3.5) and for|z|= 1 , we get

lim n→∞(nk)

1+δ kk

(P)n,k(Q)n,k(R)−1n,kzn

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≤ lim n→∞k

n(nk)−δ kk(nk)

−P k(P)n,k

(n−1)!kn−1 k k(nk)

P kk

× k(nk)

−Q k(Q)n,k

(n−1)!kn−1 k k(nk)

Q kk

× k(n−1)!kn−1(R)−1n,k(nk)Rkk k(nk)− R kk

≤ kΓ−1k (P)k kΓ−1k (Q)k kΓk(R)k

× lim

n→∞k

2n−2(nk)−δ k{

r−1 X

j=0

[max{kPk,kQk,kRk}r12]j

kj!

× (lnn)j}3

= 0, because

lim n→∞n

−δ

k(lnn)j= 0,j0, k >0. Thus

lim n→∞(nk)

1+δ kk

(P)n,k(Q)n,k(R)−1n,kz n

n! k= 0; |z|= 1,

therefore the series (3.1) is absolutely convergent for |z| = 1. Now we show that under certain condition the hypergeometric matrix k-functionFk(P, Q;R;z) is a solution of matrix differential equation of bilateral type.

Theorem 3.2. LetRis matrix inCr×r satisfyingR+nkI is invertible matrix and QR=RQ. Then Fk(P, Q;R;z) is the solution of

kz(1−kz)W00−kzP W0+W0(R−kz(Q+kI))−P QW= 0, 0≤ |z|<1 (3.6) satisfyingFk(P, Q;R; 0) =I.

Proof. By the given hypothesisQR=RQ, so we can write

Fn,k =(P)n,k(Q)n,k(R)

−1

n,k

n! =

(P)n,k(R)−1n,k(Q)n,k

n! .

Let us denote

W(z) =Fk(P, Q;R;z) =

∞ X

n=0

Fn,kzn, |z|<1. (3.7)

SinceW(z) is a power series convergent for|z|<1, so it is termwise differentiable in the given domain and

W0(z) =

∞ X

n=1

nFn,kzn−1, W00(z) =

∞ X

n=2

n(n−1)Fn,kzn−2, |z|<1.

Hence

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=

∞ X

n=2

nk(n−1)Fn,kzn−1−

∞ X

n=2

nk2(n−1)Fn,kzn−P

∞ X

n=1

nkFn,kzn

+

∞ X

n=1

nFn,kRzn−1−

∞ X

n=1

nkFn,k(Q+kI)zn−

∞ X

n=0

P Fn,kQzn,

replacingn=n+ 1 in the first and fourth summation, we obtain kz(1−kz)W00−kzP W0+W0(R−kz(Q+kI))−P QW

=

∞ X

n=1

nk(n+ 1)Fn+1,kzn−1− ∞ X

n=2

nk2(n−1)Fn,kzn−P

∞ X

n=1

nkFn,kzn

+

∞ X

n=1

nFn,kRzn−1−

∞ X

n=1

nkFn,k(Q+kI)zn−

∞ X

n=0

P Fn,kQzn

=

∞ X

n=1

{nk(n+ 1)Fn,k−nk2(n−1)Fn,k−nkP Fn,k+ (n+ 1)Fn+1,kR

− nkFn,k(Q+kI)−P Fn,kQ}zn+ 2kF2,kz−kP F1,kz+F1,kR+ 2F2,kRz

− F1,k(Q+kI)kz−P F0,kQ−P F1,kQz= 0.

By equating the coefficients of each powerzn and noting thatF

0,k=I, we get z0 : F1,kR−P IQ= 0,

z1 : 2kF2,k−kP F1,k+ 2F2,kR−F1,k(Q+kI)kz−P F1,kQ

= 2F2,k(kI+R)−P F1,k(kI+Q)−F1,k(Q+kI)k= 0 ..

. ...

⇒ Fn+1,k=

(P+nkI)Fn,k(Q+nkI)(R+nkI)−1

n+ 1 .

HenceW(z) =Fk(P, Q;R;z) is the solution of (3.6) satisfying W(0) =I.

Corollary 3.3. Let R be a matrix in Cr×r satisfying that R+nkI is invertible matrix for n ≥ 0 and let P be an arbitrary matrix in Cr×r and n be a positive integer. Then equation

kz(1−kz)W00−kzP W0+W0(R+z(n−k)kI) +nP W = 0 (3.8) has matrix polynomial solutions of degree n.

Proof. LetQ =−nI, then by theorem 3.2 the function W(z) =Fk(P,−nI;R;z) satisfies equation (3.6) forQ=−nI. Hence

W(z) =Fk(P, Q;R;z) = n

X

l=0

(P)l,k(−nI)l,k(R)l,k

l! z

l

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4. An Integral Representation of Hypergeometric matrix k-function

In this section, we define the integral representation of hypergeometric matrix k-function. If y and b are complex numbers with |y| < 1, then the Taylor series expansion of (1−ky)−kb abouty= 0 is given by [2]

(1−ky)−kb =

∞ X

n=0

(a)n,k n! y

n, |y|<1, a

C. (4.1)

Letfn,k(a) be a function defined by fn,k(a) =(a)n,k

n! y

n=a(a+k)(a+ 2k)· · ·(a+ (n−1)k)

n! y

n, a

C k >0,(4.2) for a fixed complex number y with |y|< 1. Clearly the function fn,k is an holo-morphic function of variableadefined in the complex plane fork >0. For a given closed discDα={a∈C:|a| ≤α}, we have

|fn,k(a)| ≤ (|a|)n,k|y|

n

n! ≤

(α)n,k|y|n

n! , n≥0, |a| ≤α, k >0. Since

∞ X

n=0

(α)n,k|y|n

n! ≤+∞,

so by the Weierstrass theorem for the convergence of holomorphic functions [27, 2] it follows that

g(a) =

∞ X

n=0

(a)n,k n! y

n = (1ky)−a k

is holomorphic in R fork > 0. Thus by the application of the holomorphic func-tional calculus [3], for any matrix P in Cr×r, the image of g by this functional calculus acting onP yields

(1−ky)−Pk =g(P) =

∞ X

n=0

(P)n,k n! y

n, |y|<1, (4.3)

where

(P)n,k =P(P+kI)· · ·(P+ (n−1)kI), k >0.

Suppose that Qand R are matrices in Cr×r such that QR =RQ andQ, R and R−Q are positive stable matrices. Thus by (1.5), (1.7) and with the aid of the condition thatQ,RandR−Qare positive stable matrices, we obtain

(Q)n,k(R)−1n,k = Γ−1k (Q)Γk(Q+nkI)Γk(R)Γ−1k (R+nkI),

= Γ−1k (Q)Γ−1k (R−Q)Γk(R−Q)Γk(Q+nkI)Γ−1k (R+nkI)Γk(R). (4.4) By positive stability condition of the matrices and by Lemma 2.2 it follows that

1 k

1 Z

0

tQk+(n−1)I(1−t) R−Q

k −Idt

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by (4.4) and (4.5), we get

(Q)n,k(R)−1n,k = Γ

−1

k (Q)Γ

−1

k (R−Q)[ 1 k

1 Z

0

tQk+(n−1)I(1−t) R−Q

k −Idt]Γk(R). (4.6)

Hence, for|z|<1 we can write

Fk(P, Q;R;z) =

∞ X

n=0

(P)n,k(Q)n,k(R)−1n,k

n! z n = ∞ X n=0

(P)n,kΓ−1k (Q)Γ−1k (R−Q)zn Γk(R)n!

× [1 k

1 Z

0

tQk+(n−1)I(1t) R−Q

k −Idt]

= ∞ X n=0 [1 k 1 Z 0

(P)n,kΓ−1k (Q)Γ−1k (R−Q)tQk+(n−1)I(1−t) R−Q

k −IΓk(R)zn

n! dt]. (4.7)

Now let us consider Sn,k(t) =

(P)n,kΓ−1k (Q)Γ−1k (R−Q)tQk+(n−1)I(1−t) R−Q

k −IΓk(R)zn

n! , 0≤t≤1,

and note that for 0< t <1 andn≥0, we have

kSn,k(t)k

≤(kPk)n,kkΓ

−1

k (Q)kkΓ

−1

k (R−Q)kkΓk(R)kkt Q

k−Ik(1−t) R−Q

k −Ik|z|n

n! , k >0.(4.8)

By (1.8) it follows that

ktQk−I k(1−t) R−Q

k −Ik ≤ t α(Q)

k −1(1−t) α(R−Q)

k −1[ r−1 X

j=0

(kQ−kIkr12lnt)j

kj! ]

× [ r−1 X

j=0

(kR−Q−kIkr12lnt)j

kj! ]

and noting that for 0< t <1, we have lnt < t <1 and ln(1−t)<1−t <1, hence from above expression we get

ktQk−I k(1−t) R−Q

k −Ik ≤Λt α(Q)

k −1(1−t) α(R−Q)

k −1, 0< t <1, k >0 (4.9) where

Λ = [ r−1 X

j=0

(kQ−kIkr12)j

kj! ][ r−1 X

j=0

(kR−Q−kIkr12lnt)j

kj! ]. (4.10)

Now letS be the sum of the convergent series

S= r−1 X

n=0

(kPk)n,k|z|n

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By (4.8)-(4.10), we obtain

∞ X

n=0

kSn,k(t)k ≤φ(t) = 1 k[LΛSt

α(Q)

k −1(1t) α(R−Q)

k −1],0< t <1, k >0, (4.12) where

L=kΓ−1k (Q)k kΓk−1(R−Q)k kΓk(R)k. Sinceα(Q)>0,α(R−Q)>0 andk >0, then the function φ(t) = 1k[LΛtα(kQ)−1(1−t)

α(R−Q)

k −1] is integrable and

1 Z

0

φ(t)dt=LΛSBk(α(Q), α(R−Q)).

Thus by dominated convergence theorem ([7], p.83), the series and the integral can be computed in (4.7) and usingQR=RQ, we can write

Fk(P, Q;R;z)

= 1 k

1 Z

0

{

∞ X

n=0

((P)n,k(tz) n

n! )t Q

k−I(1−t) R−Q

k −I}dtΓ−1

k (Q)Γk(R−Q)Γk(R). (4.13) Now by (4.3), we obtain

∞ X

n=0

(P)n,k(tz)n

n! = (1−ktz)

−P

k, |z|<1, 0< t <1, (4.14) and (4.13) becomes

Fk(P, Q;R;z)

= Γ−1k (Q)Γk(R−Q)Γk(R) 1 k

1 Z

0

tQk−I(1−t) R−Q

k −I(1−ktz)− P

kdt. (4.15)

Summarizing, the following result has been established:

Theorem 4.1. Let P,Q andR be matrices inCr×r such that QR=RQand Q, R,R−Qare positive stable matrices. Then for|z|<1 it follows that;

Fk(P, Q;R;z) = Γ−1k (Q)Γk(R−Q)Γk(R)[1 k

1 Z

0

tQk−I(1−t) R−Q

k −I(1−ktz)− P kdt].

(4.16)

Corollary 4.2. Let P,QandR be matrices in Cr×r and let ˆ

α(Q, R) = min{α(Q), α(R), α(R−Q)} andn1=n1(Q, R) = [|α(Q, R)ˆ |] + 1, where

[|α(Q, R)ˆ |]denotes the entire part function. Suppose that QR=RQ, and σ(Q) ⊂ R∼ {−n;n≥n1, n∈Z}

σ(R−Q) ⊂ R∼ {−n;n≥n1, n∈Z}

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Then for |z|<1, we have

Fk(P, Q+n1kI;R+ 2n1kI;z) = Γ−1k (Q+n1kI)Γk(R−Q+n1kI)

× Γk(R+ 2n1kI)

× 1

k

1 Z

0

tQk+(n−1)I(1t) R−Q

k +(n−1)I

× (1−ktz)−Pkdt.

Proof. Consider the matrices P, ˆQ = Q+nkI, ˆR = R+nkI and ˆR, ˆQ, ˆ

R−Qˆ =R−Q+n1kI are positive stable matrices. The result is now a

conse-quence of theorem 4.1.

Conclusion. In this paper, the authors conclude that for each positive value ofkthere exist gamma, beta and hypergeometric matrix arguments which are the improved generalized version of the said classical functions with matrix arguments. Obviously the substitutionk= 1 will lead to the results of the said classical func-tions with matrix arguments.

Acknowledgements

The authors would like to express profound gratitude to referees for deeper review of this paper and the referee’s useful suggestions that led to an improved presenta-tion of the paper.

Conflict of Interests

The author(s) declare(s) that there is no conflict of interests regarding the publi-cation of this article.

References

[1] A.G. Constantine, R.J. Muirhead,Partial differential equation for hypergeometric functions of two arguments matrix, J. Multivariate Anal. 3(1972), pp.332-338. Press, 1990.

[2] R. Diaz, E. Pariguan ,On hypergeometric functions and pochhammerk-symbol, Divulgaciones Matemticas, Vol.15 No. 2(2007),pp.179-192.

[3] N. Dunford, J. Schwartz,Linear Operator, vol. I. Interscience, New York, 1957.

[4] A.J. Dur´an, W. Van Assche,Orthognal matrix polynomial and higher order recurrence rela-tions, Linear Algebra Appl. 219 (1995), pp. 261-280.

[5] A.J. Dur´an,Markov theorem for orthognal matrix polynomials, Can. J. Math. 48 (1996), pp. 1180-1195.

[6] A.J. Dur´an, P. L´opez-rodriguez,Orthognal matrix polynomial: zeros and Blumenthal’s theo-rem, J. Approx. Theory 84 (1996), pp. 96-118.

[7] G.B. Folland,Fourier Analysis and its Application, Wadworth and brooks, Pacific Grove, CA, 1992.

[8] G. Golub, C.F. Van Loan,Matrix Computation, The Johns Hopkin Univ. Press, Baltimore, MA, 1989.

[9] C.S. Herz,Bessel functions of matrix argument, Ann. Math. 61(1955), pp. 474-523. [10] E. Hille,Lecture on Ordinary Differential Equations, Addison-Wesley, New York 1969. [11] A.T. James, Special function of matrix and single argument in statistics in: Theory and

Application of Special Functions, R.A.Askey (Ed.), Acadamic Press, New York, 1975, pp. 497-520.

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[13] L. J´odar, R. Company, E. Navarro,Laguerre matrix polynomial and system of second order differential equations, Appl. Numer. Math. 15 (1994), pp. 53-63.

[14] L. J´odar, R. Company, E. Ponsoda,Orthognal matrix polynomials and system of second order differential equations, Diff. Equations Dynam. Systems 3(3) (1995), pp. 269-288.

[15] L. J´odar, R. Company,Hermite matrix polynomial and second order matrix differntial equa-tions, Approx. Theory Appl. 12(2) (1996), pp. 20-30.

[16] L. J´odar, J. Sastre,On the Laguerre matrix polynomials, Utilitas Math. 53 (1998), pp. 37-48. [17] L. J´odar, J.C Cort´es, Some properties of gamma and beta matrix functions, Appl. Math.

Lett. 11(1) (1998), pp. 89-93.

[18] L. J´odar, J.C. Cort´es,On the hypergeometric matrix function, J. Comp. Appl. Math. 99 (1998), pp. 205-217.

[19] Y.L. Luke,The Special Functions and their Applications, 2 vols. Acdamic Press, New York, 1969.

[20] S. Mubeen and G. M. Habibullah, An integral representation of some k- hypergeometric functions, Int. Math. Forum, vol. 7, pp. 203-207, 2012.

[21] S. Mubeen , M. Naz , G. Rahman,A note onk-hypergeometric diffrential equations,Journal of Inequalities and Special Functions ISSN: 2217-4303, URL: http://www.ilirias.com Volume 4 Issue 3(2013), pp. 38-43.

[22] S. Mubeen, G. Rahman, A. Rehman, M. Naz, Contiguous function relations for k-hypergeometric functions,ISRN Mathematical Analysis Volume 2014, Article ID 410801, 6 pages.

[23] S. Mubeen, M. Naz, A. Rehman, G. Rahman, Solutions of k-hypergeometric differential equations, Journal of Applied Mathematics Volume 2014, 13 pages.

[24] S. Mubeen, S. Iqbal, G. Rahman,contiguous function relations and integral representation of Appellk-seriesF1,k, International Journal of Mathematical Research, 4(2015), pp. 53-63. [25] S. Mubeen, G. Rahman, M. Arshad,Onk-gamma,k-beta matrices and their properties, J.

Math. Comput. Sci. 5 (2015), pp. 647-657.

[26] E. D. Rainville, Special Funtions, Macmillan Company, New York, 1960. [27] S. Saks, A. Zygmund,Analytic Functions, Elsevier, Amsterdam, 1971.

[28] J.B. Seaborn,Hypergeometric Functions and their Applications, Springer, New York, 1991. [29] N.M. Temme,Special Functions, Wiley, New York, 1996.

Gauhar Rahman

Department of Mathematics, International Islamic University, Islamabad, Pakistan.

E-mail address:[email protected]

Abdul Ghaffar

Department of Mathematics, Balochistan University of Information Technology, En-gineering and Management Sciences

E-mail address:[email protected]

Sunil Dutt Purohit

Department of HEAS (Mathematics), Rajasthan Technical University, Kota-234010, In-dia.

E-mail address:sunil−a−[email protected]

Shahid Mubeen

Department of Mathematics, University of Sargodha, Sargodha 40100, Pakistan.

E-mail address:[email protected]

Muhammad Arshad

Department of Mathematics, International Islamic University, Islamabad, Pakistan.

References

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