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(1)

A NNALI DELLA

S CUOLA N ORMALE S UPERIORE DI P ISA Classe di Scienze

M. A. A L B ASSAM

Some operational properties of the H-R operator

Annali della Scuola Normale Superiore di Pisa, Classe di Scienze 3

e

série, tome 27, n

o

3 (1973), p. 491-506

<http://www.numdam.org/item?id=ASNSP_1973_3_27_3_491_0>

© Scuola Normale Superiore, Pisa, 1973, tous droits réservés.

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Article numérisé dans le cadre du programme Numérisation de documents anciens mathématiques

http://www.numdam.org/

(2)

OF THE H-R OPERATOR by

M. A. AL BASSAM

Department of Mathematics, Kuwait University

1.

Introduction.

The work of this article is

closely

related to the

study

revealed

by

papers

[1] ]

and

[2].

In

[1]

the author has studied some

properties

of what

he called « H-R

transform)*,

which is associated with the

concept

of gene- ralized derivative and

integral.

In fact the linear

operator

of the

transform,

or the H-R

operator,

may

simply

be considered as an

integro

differential

operator

of

generalized

order. Some writers refer to the H-R transform as

the « fractional derivative and

integral », [3], [4].

The H-R transform has been

by

the

following:

DEFINI1.’ION.

If f (x)

is a real valued function contained in on the

I

interval a x

b,

and Re

(a -~- n) ~ 0,

then

or

(n

==

1, 2, ...),

where

Dx

is the nth derivative

operator

with

respect to x,

D) f, 0,,nl

is the set of functions with continuous nth derivative on

[a, b]

and is the conventional

symbol representing

Gamma function of x.

Pervenuto alla Redazione il 14 Marzo 1972.

(3)

The first form of the above definition can be written as

Based on this

definition,

it has been shown in

[1]

that:

THEOREM 1.

(i) If f (x)

is a function

belonging

to on

[a, b]

and

Re

(a + m) &#x3E; 0,

then

(ii)

is a function in on

[a, b],

then

From

(i)

and

(ii),

it follows that

THEOREM 2. If

f(x)

and

g(x) satisfy

the conditions of the definition and A is a

number,

then

(ii) If f (x)

ie a

polynomial

of

degree n and Re (a) &#x3E; 0,

then

(ii) represente

a

special

case of a

generalization

of Leibnitz’ rule of diffe-

rentiation of

product

of two functions.

THEOREM 3.

(i)

If

x &#x3E; a

where a is a real

number,

and

~B ~ - m ~

a

negative integer),

then

for all values of a and

P.

(4)

(ii) If fl

= - n

(a negative integer),

Re

(a + m) &#x3E;

0

(m

=

0, 1, 2, ...),

then

for all values of a, where lnu du.

THEOREM 4. The relation

holds if

negative integer,

and

Another

property

needs to be mentioned is that

if fl -* - n

and

f (x)

satisfies the conditions of

(Theorem 4),

then

for all values of 0153 and

~3.

then this relation holds

if/~(~)==0

for

(p,

=

0,1, 2,..., m - 1).

x

The work of this paper deals

mainly

with

operations

of

Ia,

the gene-

a

ralized

integro-differential operator,

on certain

types

of functions

belonging

to the set Tq-Functions studied in

[2].

So it may be useful to

give

defini-

tions and some

properties

of functions related to such

operations.

(5)

The function

Ea (~, ; x - a), simply

denoted

by

has been defined

by

where 1 is a number. Also we have defined

It

follows,

from these

definition,

that

Other

functions

have been defined as follows :

(6)

From the above definitions we have the

following properties :

In what

follows,

the valuse of a and conditions

imposed

on

f (x)

will

x

be similar to those mentioned

by

definition of

Ia f,

and for which the

a

operation

has a

meaning.

Also when and

where

belong

to Ta

Functions.

then the

product

FG

in

T,2, (see [2]),

where

and

consequently

each one of these series is

absolutely

and

uniformly

con-

vergent.

Thus term

by

term

integration

and differentiation can be

perfor-

med.

Therefore,

the

operations

carried out in the

following

sections are

justified

and

permissible.

2.

Some Operational Properties.

According

to what has been written in the

previous

section we have

Therefore we have the

following

(7)

DEFINITION.

(P-1 ) :

If A is a

number,

y we have

and in

particular,

when

f (x) -1,

To show

this,

we have

from which we obtain

(P-1).

The other relation is obtained

by putting f (x) =-= 1

in

(P-1).

This relation follows from

Also we notice that

(8)

To show

this,

we have

This may be shown as follows :

(ii)

Also it can be obtained

by

direct

expansion :

(9)

(P~s) :

Extension of

(P-3).

If n is a

positive integer

such

that n &#x3E; 1,

then

(10)

From

(P-7)

and

(P-8)

we may conclude that

(P.ll) : Writing

and

using property (P-9),

then we would have

In

general

we find that

and

where

(n

=

0,1, 2, ...)

and

( p == 1, 2, 3, ...).

(11)

3.

Operations

on some

Special

Ta.Functions

Consequently

we have

Also if we let

where N _ n

and

(ax)

is a sequence of

numbers,

we would have

where

(P- 13):

By applying

Theorem 2

(ii)

we find that

It caa also be shown that for k

~:&#x3E; 1,

(12)

for the left hand

side, according

to

(P-13),

is

equal

to

Also we find that

This

property

can be

easily

obtained

by applying

to the

right-hand

side of

THEOREM 2

(ii).

In

general,

for k &#x3E;

2,

we have

In a similar way as above it has been found that:

(13)

A

generalization

of the above established formulas may be

given by (P-16) :

(A)

For k

(B) For k &#x3E; n~

we have

from which have for n

(P-17) :

From

properties

of the functions

Sa ; ~ , Oa; Å’

and we

have the

following :

It would be sufficiente to show the

validity

of the first two relations

as the others follows in a similar way. We have

(14)

Also we have

4.

Some Applications.

The

operational properties

of the

integro

differential

operator

of gene- ralized order may be used to deal with

solving

differential or

integro diffe-

rential

equations

of

generalized

order in a similar way the

ordinary

diffe-

rential

operators

are used in

solving ordinary

linear differential

equations.

This may be

explained by

the

following:

EXAMPLE 1. Consider the differential

equation

of

generalized

order

&#x3E; 07

0

where A is a

parameter

and

f (t)

is

integrable

function on a t b. This

equation

can be written as

where C is an

arbitrary

constant. Now if we

put

the

equation

in the form

10. Anntdi delta Scuola Norm. Sup. di Piea.

(15)

then

Thus, denoting

y

(x) by Y. (x)

we would obtain the solutions

REMARK. It may be

interesting

to note that when a

=1, equation (i)

is reduced and

(ii)

is reduced to

EXAMPLE 2. Solution of

Equations

with Constant Coefficients. Let

In order to solve this

equation,

we notice that if we assume that the

equation

has solutions of the form

B.;A,

then we have

where

J?(A)==0

is similar to the characteristic

equation

associated with an

ordinary

linear differential

equation.

Thus will be a solution of the differential

equation

of

generalized

order

(iii)

if A is chosen as a root of the

equation

(16)

If this

equation

has n-distinct real

roots,

... ,

1n,

then the get neral solution

Ya (x)

may be

given by

where

Cp,

p

= 1, 2,..., n,

are

arbitrary

constants.

The same form of

general

solution may be obtained if 2k

n

of the roots are

complex

and it may be

expressed

in terms of functions of the forms

Sa ; ~ ,

and

00;.B.

If the

equation

has

n-repeated roots, say A

= r, then the

equation

may take the form

By (~~16)

we have

for

(k

=

0,1, 2,..., n -1).

Therefore

Ya (x)

may take the form

where the are

arbitrary

constants.

Other cases related to the roots of the characteristic

equation

may be dealt with in a similar way.

(17)

BIBLIOGRAPHY

[1] M. A. AL-BASSAM: Some

properties

of

Holmgren-Rtesz

transform, Annali della Scuola Normale

Superiore

di Pisa, Scienze Fisiche e Matematiche - Serie III. Vol. XV.

Fasc. I.II (1961), pp. 1-24.

[2] M. A. AL-BASSAM: On

functional representation by

a certain type of

generalized

power series, Annali della Scuola Normale

Superiore

di Pisa, Scienze Fisiche e Matematiche - Serie III. Vol. XVI. Fasc. IV (1962), pp. 351-366.

[3] G. H. HARDY: Some properties of

integral

of

fractional

order, Messenger of Mathema- tics, Vol. 47, (1913), pp. 145-150.

[4] G. H. HARDY and J. E. LITTLEWOOD: Some properties of

fractional integrals,

Mathe-

matische Zoitschrift, Vol. XXVII, (1927), pp. 565-606.

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