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ON SOME FRACTIONAL INTEGRAL FORMULAE INVOLVING THE

MULTIVARIABLE I -FUNCTION AND A GENERAL CLASS OF POLYNOMIALS

Yashwant Singh1, Harmendra Kumar Mandia2

1,2 Department of Mathematics,

1Governmant college Kaladera,Jaipur(Rajasthan), India

2Seth Motilal (P.G.) College, Jhunjhunu(Rajasthan), India

1[email protected]

2[email protected]

Abstract— In the present paper, the authors have obtained two fractioal integral formulae involving the product of a general class of polynomials and the multivariable

I

-function. On account of the most general nature of these functions, a number of results (known and new) follow as special cases of our formulae. In the end, we obtain a fractional integral formula involving the laguerre and the hermite polynomials as a simple special case of our main formula.

Keywords- Riemann-Liouville Fractional Integral Operator, Multivariable

I

-function, General Class of Polynomials, Mellin- Barnes contour Integral

(2000 Mathematics subject classification: 33C99).

I. INTRODUCTION

In the present paper the fractional integral operator will be defined and represented as follows:

( )1 ( )

1

( ) , Re( ) 0

( )

x

v v

c x

c

I f x x t f t dt v

v

 

 

(1.1)

The special case of the above fractional integral for

0

c

is the Riemann-Liouville fractional integral operator and will be written as

I

xv

f x ( )

.

Also, the fractional integral operator investigated by Erdelyi-Kober will be defined and represented as follows:

 

1

, 1 1

0

( ) ( ) ( ) , Re( ) 0, 0

( )

v x

v v

x

I f x x x t t f t dt v

v

  

  

 

(1.2)

Clearly, this is a generalization of Riemann-Liouville fractional integral operator.

The multivariable

I

-function introduced by Prasad [2] will be define and represent it in the following manner :

 

2

( )( )( )( )

2 2

0, :...:0, :( ', '):...: , 1

,...,

, :...: , :( ', '):...: ,

r r

r

r r

r r

n n m n m n

r p q p q p q p q

I z zI

( ) ( ) ( )

' '' ' ' '

2 2 2 1,2 1, 1, ' 1,( )

( ) ( ) ( )

' '' ' ' '

2 2 2 1,2 1, 1, ' 1,( )

( , , ) :...:( , ,..., ) :( , ) :...:( , )

1

,...,

( , , ) :...:( , ,..., ) :( , ) :...:( , )

r r r

j j j p rj rj rj pr j j p j j pr

r r r

j j j q rj rj rj qr j j q j j qr

a a a

r b b b b

z z

   

 

 

 

1

1

1 1 1 1 1

1 ... ( )... ( ) ( ,..., ) ,..., ...

(2 )

r

r

s s

r r r r r

r

L L

s s s s z z ds ds

w   

   

(1.3) Where

( 1) w  

   

   

( ) ( )

( ) ( )

( ) ( )

( ) ( ) ( ) ( )

1 1

( ) ( ) ( ) ( )

1 1

1

( ) (1, 2,..., )

1

i i

i i

i i

m n

i i i i

j j i j j i

j j

i i q p

i i i i

j j i j j i

j m j n

b s a s

s i r

b s a s

 

 

    

  

    

 

 

(1.4)

3 2

3 2

2 3

2 3

( ) ( )

2 2 3 3

1 1

1 1

1 2 3

( ) ( )

2 2 3 3

1 1

1 1

1 1

( ,..., )

n n

i i

j j i j j i

i i

j j

r p p

i i

j j i j j i

i i

j n j n

a s a s

s s

a s a s

 

 

   

   

         

   

            

   

 

 

 

 

2

( ) 1 1

2

( ) ( ) ( )

2 2

1 1 1

1 1 1

... 1

... 1 ... 1

r

r r

r

n r

i

rj rj i

j i

p r q q r

i i i

rj rj i j j i rj rj i

i i i

j n j j

a s

a s b s b s

  

 

 

    

 

     

                   

  

  

(1.5)

(2)

( ) ( ) ( ) ( )

, , , ( 1,..., )( 1,..., )

i i i i

j j kj kj

i r k r

     

are positive numbers,

( ) ( )

, ( 1,..., ), , ( 2,..., )

i i

j j kj kj

a b ir a b kr

are complex numbers and here

( ) ( ) ( ) ( )

, , , ( 1,..., ), , , ( 2,..., )

i i i i

k k k

m n p q ir n p q kr

are non-negative integers where

( ) ( ) ( ) ( )

0  m

i

q

i

, 0  n

i

p

i

, q

k

 0, 0  n

k

p

k

. Here

( ) i

denotes the numbers of dashes. The contours

L

i

in the complex

s

i

-plane is of the Mellin-Barnes type which runs from

  w

to

  w

with indentations, if necessary, to ensure that all the poles of

  b

( )ji

 

( )ji

s

i

 j1,..., m

( )i

are

separated from those of

 

( ) 1

1 1,...,

r i

rj rj i r

i

as j n

 

     

  

.

For further details and asymptotic expansion of the

I

-

function one can refer by Prasad [2].

In what follows, the multivariable

I

-function defined by [2] will be represented in the contracted notation:

 

 

 

( ) ( )

  

2

( ) ( )

2 2

0, :...:0, : ', ' :...: ,

, :...: , : ', ' :...: , 1

,...,

r r

r

r r

r r

n n m n m n

p q p q p q p q r

I z z

Or simply by

I z

1

,... z

r

.

According to the asymptotic expansion of the gamma function, the counter integral (1.3) is absolutely convergent provided that

arg 1 , 0

i

2

i i

z   U U

;

i 1  , 2, . . . . , r

(1.6)

Where

( ) ( )

( ) ( )

( ) ( ) ( ) ( )

1 1 1 1

i i

i i

i i

p q

n m

i i i i

i j j j j

j j n j j m

U    

       

3 3

2 2

2 3

( ) ( ) ( ) ( )

2 2 3 3

1 1 1 1

( ) ( )

n p

n p

i i i i

j j j j

j j n j j n

   

   

       

( ) ( )

1 1

... ( )

r r

r

n p

i i

rj rj

j j n

 

 

    

3 2

( ) ( ) ( )

2 3

1 1 1

( ... )

q r

q q

i i i

j j rj

j j j

  

      

(1.7)

The asymptotic expansion of the

I

-function has been discussed by Prasad [2]. His results run as follow:

1

1 1 1

[ ,...,

r

] 0( ...

r r

), max{ ,...,

r

} 0

I z zz

z

z z

Where

( ) ( )

min Re(

i

/

i

)

i

b

j j

  

,

1 , . . . . ,

( )i

jm

;

i 1  , . . . . , r

And

1

1 1 1

[ ,...,

r

] 0( ...

r r

), min{ ,...,

r

}

I z zz

z

z z  

Where

( )

( )

max Re( 1 )

i j

i i

j

a

 

;

1 , . . . . ,

( )i

jn

,

i 1  , . . . . , r

The details of the function can be found in the paper of Prasad [2].

Again we shall use the following notation:

 

' ( )

1,

1 2

2 2

( ) '

1,

; ,..., ,...

0, :...:0, :...

, :...: , :...

; ,..., ,...

r

j j j u

r

r r

r r

j j j v

z

n n u

p q p u q v z

v

I

 

 

 

 

 

 

For the multivariable

I

-function given by (1.3)

Srivastava ([4], p.1, eq. (1)) introduced a general class of polynomials

S

nm

[ ] x

defined by means of the following equation:

, 0

( )

[ ] , 0,1, 2,...

!

nm

m mk k

n n k

k

S x n A x n

k

   

(1.8)

Where

m

is an arbitrary positive integer and the coefficients

A

n k,

( , n k  0)

are arbitrary constants, real or complex. On specializing these coefficints

A

n k,

; S

nm

yields a number of known polynomials as special cases. These include, among others, the Hermite polynomials, the Jacobi polynomials, the Laguerre polynomials, the Bessel polynomials, the Gould-Hopper polynomials, the Brafman polynomials and many others.

II. FRACTIONAL INTEGRAL FORMULAE

( ) ( )

m u

( ) (

v

)

w

c

I

x

x

x  

x  

S

n

  ax x   x    

1 1 1

' ' ' '

'

( ) ( )

1 u

( ) (

v

) ,...,

w

m u v w

S

n

  bx x   x      I z xx   x  

z x

r ur

( x ) (

vr

x )

wr

 

=

' '

'

' ' , ', '

, , 0 0 ' 0

( ) ( ') '

n n

m m

k k

mk m k n k n k

s l t k k

x n n A A a b

 

 

 

 

 

  

(3)

' '

' ' 1 ' ' 1

( 1) ( )

! '! ! ! ( ) ( ) !

s s uk u k l t s

k k wk w k

x c x

k k l t s s

 

 

 

  

 

 

1 1 1 1 1 2

2 2

1

( ' ' ; ,..., ),

0, :...:0, 3:...

, :...: 3, 3:...

( ' ' ; ,..., ),

r

v w u

r

v w u

r r r r r

r

r

uk u k l t u u

z x

n n

p q p q

z x

s uk u k l t u u

I

 

 

    

    

 



1 1

1 1

( ' '; ,..., ),( ' '; ,..., );...

( ' '; ,..., ),( ' '; ,..., );...

r r

r r

vk v k v v wk w k w w

l vk v k v v t wk w k w w

    

    



(2.1)

Provided that

(i)

 

Re( ) v  0; min u v w u v w u v w

i

, ,

i i

, , , , ', ', '  0, i  1, 2,..., ; r

max | arg x ,| arg x

 

      

         

 

and the

I

-function

of

r

variables involved in (2.1) satisfy the usual convergence and existance conditions.

(ii)

( )

( )

1 ( ) 1

Re( ) min Re 1 0

i

r i

j

i i

i j m j

u d

 

   

 

               

(iii) The series occuring on the right-hand side of (2.1) is absolutely convergent.

,

( ) ( )

m u

( ) (

v

)

w

x n

I

 

x

x  

x  

S   ax x   x    

1 1 1

' ' ' '

'

( ) ( )

1 u

( ) (

v

) ,...,

w

m u v w

S

n

  bx x   x      I z xx   x  

( ) ( )

r r r

u v w

z x

r

x   x    

=

' '

'

' ' , ', '

, 0 0 0 ' 0

( ) ( ') '

n n

m m

k k

mk m k n k n k

l t k k k

x n n A A a b

 

 

 

   

 

   

' '

' ' 1 ' ' 1

( 1)

! '! ! !

s uk u k l t

k k wk w k

x

k k l t

 

 

1 1 1 1 1 2

2 2

1

(1 ' ' ; ,..., ),

0, :...:0, 3:...

, :...: 3, 3:...

( 1 ' ' ; ,..., ),

r

v w u

r

v w u

r r r r r

r

r

uk u k l t u u

z x

n n

p q p q

z x

v uk u k l t u u

I

   

   

     

       

 



1 1

1 1

( ' '; ,..., ),( ' '; ,..., );...

( ' '; ,..., ),( ' '; ,..., );...

r r

r r

vk v k v v wk w k w w

l vk v k v v t wk w k w w

    

    



(2.2) Where

( )

( )

1 ( ) 1

0, Re( ) min Re

i

r i

j

i j m i

i j

u d

  

 

   

 

                

The series occuring on the right-hand side of (2.2) is absolutely convergent and the set of conditions (i) specified in the formula (2.1) are satisfied.

Proof of (2.1):

To establish the fractional integral formula (2.1), we first express the general class of polynomials

S

nm

[ ] x

and

'

'

[ ]

m

S

n

x

occuring on its left-hand side in the series form given by (1.8) and replace the multivariable

I

-function occuring therein by its well known Mellin-Barnes contour integral [5].

The left-hand side of (2.1) (say

) takes the following form:

,

0

( )

( ) ( )

!

nm

mk

c x n k

k

I x x x n A

k

     

' '

' ' ', ' ' 0

( ')

( ) ( )

'!

nm

u v w k m k

n k k

ax x x n A

  k

    

  

1

' ' ' '

1

( ) ( ) 1 ... ( ,..., )

(2 )

r

u v w k

r r

L L

bx x x

  i   

    

   

1 1 1 1

1

( ).... ( )

1 r r

z x

1 u

( x ) (

v

x )

w

           

( ) ( )

r 1

...

r r r

u v w

r r

z x xx

dd

   

 

(2.3)

Now interchanging the order of

i

-integrals and the fractional integral involved in (2.3), collecting powers of

, ( )

x x  

and

( x   )

in the expression thus obtained, making use of the following binomial expressions for

( x   )

and

( x   )

 

0

( ) ; | | 1

l

l l

x x

x

 

   

           

 

0

( ) ; | | 1

t

t t

x x

x

 

   

      

   

And changing the order of

i

-integrals and

l t ,

-series,

which is easily seen to be permissible under conditions stated, we get after a little simplification the following result:

' '

' '

, ', '

, 0 0 ' 0

( ) ( ')

! '! '

n n

m m

mk m k

n k n k

l t k k

n n

k k A A

 

   

 

    

' ' ' '

! !

vk v k l wk w k t

l k

 

1

1

1 ... ( ,..., ) (2 )

r

r r

L L

i   

  

1 1 1

1

( ).... ( )

1 r r

z

1 v w

... z

r vr wr r

               

' ' 1 1 ...

1 1

1 1

' ' ... 1

' ' ... 1

r r r r

uk u k u u l t v

c x

r r

vk v k v v

I x vk v k v v l

  

  

     

      

       

 

1 11 1

1

' ' ... 1

' ' ... 1 ...

r r

r r r

wk w k w w

d d

wk w k w w t

  

 

  

      

       

(2.4)

(4)

Now making use of the familiar formula ([],p.22)

  

0

( 1) 1 ( )

, Re( ) 1

( ) 1 !

s s v s

v c x

s

x c x I x

v s s v s

 

   

  

    

(2.5)

In eq. (2.5), changing the order of

s

-series and

i

- integrals, which is also permissible under conditions stated and interpreting the resulting multiple Mellin-Barnes contour integral so obtained in terms of

I

-function of

r

variables, we finally arrive at the desired result.

In order to establish the fractional integral formula (2.2) (involving Erdelyi-Kober operator defind by (1.2), we proceed along the lines followed in (2.1) and make use of the result

 

,v

, Re( )

x

I x x

v

 

 

 

 

  

  

(2.6) In place of formula (2.5).

3. Special Cases

Each of the fractional integral formulae (2.1) and (2.2) has two-fold generality. Not only do the general class of polynomials involved in these results reduce, under special cases, to a large spectrum of polynomials defined by Srivastava [4], the multivariable

I

-function occuring herein can also be suitably specilized to a remarkable wide variety of useful functions. A number of results (known and new) follow as special cases of these formulae.

If in (2.1) and (2.2), we put

2

...

r 1

0

2

...

r 1

,

2

...

r 1

0

n   n

  p   p

q   q

, the multivariable

I

-function reduces to multivariable

H

- function and we get result given by Gupta et. al. [1]

( ) ( )

m u

( ) (

v

)

w

c

I

x

x

x  

x  

S

n

  ax x   x    

1 1 1

' ' ' '

'

( ) ( )

1 u

( ) (

v

) ,...,

w

m u v w

S

n

  bx x   x      H z xx   x  

z x

r ur

( x ) (

vr

x )

wr

 

=

' '

'

' ' , ', '

, , 0 0 ' 0

( ) ( ') '

n n

m m

k k

mk m k n k n k

s l t k k

x n n A A a b

 

 

 

 

 

  

' '

' ' 1 ' ' 1

( 1) ( )

! '! ! ! ( ) ( ) !

s s uk u k l t s

k k wk w k

x c x

k k l t s s

 

 

 

  

 

 

1 1 1 1 1

1

( ' ' ; ,..., ),

3:...

3, 3:...

( ' ' ; ,..., ),

r

v w u

vr wr ur r

r

uk u k l t u u

z x

n

p q

z x

s uk u k l t u u

H

 

 

    

    

 



1 1

1 1

( ' '; ,..., ),( ' '; ,..., );...

( ' '; ,..., ),( ' '; ,..., );...

r r

r r

vk v k v v wk w k w w

l vk v k v v t wk w k w w

    

    



(3.1)

Provided all the conditions are satisfied given in (2.1), [1].

,

( ) ( )

m u

( ) (

v

)

w

x n

I

 

x

x  

x  

S   ax x   x    

1 1 1

' ' ' '

'

( ) ( )

1 u

( ) (

v

) ,...,

w

m u v w

S

n

  bx x   x      H z xx   x  

( ) ( )

r r r

u v w

z x

r

x   x    

=

' '

'

' ' , ', '

, 0 0 0 ' 0

( ) ( ') '

n n

m m

k k

mk m k n k n k

l t k k k

x n n A A a b

 

 

 

   

 

   

' '

' ' 1 ' ' 1

( 1)

! '! ! !

s uk u k l t

k k wk w k

x

k k l t

 

 

1 1 1 1 1

1

(1 ' ' ; ,..., ),

3:...

3, 3:...

( 1 ' ' ; ,..., ),

r

v w u

vr wr ur r

r

uk u k l t u u

z x

n

p q

z x

v uk u k l t u u

H

   

   

     

       

 



1 1

1 1

( ' '; ,..., ),( ' '; ,..., );...

( ' '; ,..., ),( ' '; ,..., );...

r r

r r

vk v k v v wk w k w w

l vk v k v v t wk w k w w

    

    



(3.2)

Provided all the conditions are satisfied given in (2.2), [1].

If we take

c  0

in (3.1) and make use of the following result:

 

' ( )

1

1,

( ) '

1 1,

; ,..., :

0, :

, 1: ( ; ,..., ), ; ,..., :

0

( 1) ( )( ) !

r

j j j p

r

r j j j

r q

s z a

n

p q z s k u u b

s

s s v s H

 

 

  

   

= 1

' ( )

1,

 

' ( )

1 1,

; ,..., :

0, :

, 1: ( ; ,..., ), ; ,..., :

r

j j j

p r

r j j j

r q

z a

n

p q z v k u u b

H

 

 

 

 

We arrive at the following fractional integral formula after a little simplification:

( ) ( )

m u

( ) (

v

)

w

c

I

x

x

x  

x  

S

n

  ax x   x    

1 1 1

' ' ' '

'

( ) ( )

1 u

( ) (

v

) ,...,

w

m u v w

S

n

  bx x   x      H z xx   x  

z x

r ur

( x ) (

vr

x )

wr

 

=

' '

'

' ' , ', '

, 0 0 ' 0

( ) ( ') '

n n

m m

k k

mk m k n k n k

l t k k

x n n A A a b

 

 

 

   

 

  

' '

' ' 1 ' ' 1

( 1) ( )

! '! ! !

s s uk u k l t

k k wk w k

x c x

k k l t

 

 

1 1 1 1 1

1

( ' ' ; ,..., ),

3:...

3, 3:...

( ' ' ; ,..., ),

r

v w u

vr wr ur r

r

uk u k l t u u

z x

n

p q

z x

v uk u k l t u u

H

 

 

    

     

 



1 1

1 1

( ' '; ,..., ),( ' '; ,..., );...

( ' '; ,..., ),( ' '; ,..., );...

r r

r r

vk v k v v wk w k w w

l vk v k v v t wk w k w w

    

    



(3.3)

Where the conditions of validity directly obtainable from those mentioned with (2.1) are satisfied.

References

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