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(1)

A DISTRIBUTIONAL HARDY TRANSFORMATION

R.S. PATHAK

Department of Mathematics Banaras Hindu University

Varanasl, India

J.N. PANDEY

Department of Mathematics

Carleton Unlverslty Ottawa, Canada (Received

January

23,

1979)

_ABSTRACT: The Hardy s F-transform

0

is extended to distributions. The corresponding inversion formula

f(x)

C (ix) t

F(t)dt

0

is shown to be valid in the weak distributional sense. This is accomplished by transferring the inversion formula onto the testing function space for the generalized functions under consideration and then showing that the limiting

(2)

process in the resulting formula converges with respect to the topology of the testing function space.

KEY WORDS AND PHRASES. Integral Transform, Hardy Transform, Hankel Transform,

%strib’zio ns’ Genzed Funcio ns

AMS (MOS) SUBJECT CLASSIFICATION (1970) CODES. Primary 44A20, Secondary 46F05.

I. INTRODUCTION.

The Hardy transforms with their inversion formulae are represented by the following two integral equations:

f(x) F (tx)tdt

C (ty)yf(y)dy

0 0

and

where 0 0

()

(2)

and

C

(z) cosp

J

(z) +

slnp Y

(z)

F(p + m+ I) F(P + m+ + I)

m=0

22

-v-2p s

+ 2p I, v(z)/ {r(p) r(v +p)} [2,

p.

40].

(3)

(4)

The theory of the inversion formulae (i) and

(2)

has been given by Cooke

[I].

The Hankel transform with its inversion formula can be deduced as a special case of both

(I)

and

(2)

by taking p 0. The Y-transform

[3,

p.

93]

is a special case of (i) whereas H-transform

[3,

p.

155]

is a special case of

(2)

for p

%.

Recently the inversion formula

(I)

was proved to be valid for the generalized function space

H’ (I)

by Pathak and Pandey

[7]

in the weak distributional sense.

It turns out that the kernal y F

(ty)

of

F

-transform does not belong to the space

(3)

H

(I)

and therefore the inversion formula

(2)

cannot be proved to be valid for the space of distributions directly as a corollary to theorems proved in

[7].

We will therefore extend briefly the inversion

formula (2)

to a generalized function

space essentially by following the techniques and results proved in

[7].

2. TESTING FUNCTION SPACE H’p

(I).

For

-1/2 _< _< 1/2

and real p let F

(z)

be the function defined in

(4)

and let be a fixed number satisfying

+ +

2p

>_

0.

Assume that

8

is also a fixed number satisfying

_>

max (v

+

2p 2,

-1/2).

For each k 0,

I,

2, define a positive and continuous function

k(X)

on

satisfying

k(x)

x

2k+

O<x<l

x-8

-2 x>l.

An infinitely differentiable complex-valued function

(x)

defined over

I

is H ,P

said to belong to the space

(I)

if ,8

k ()

sup

k(X) Akx ( )

x

<

O<x<

for each k 0, i, 2, 3, where A stands for the differentiation operator x

2

D

+-

D D

x It can be readily seen that HV’p

(I)

is a vector

x x x dx ,8

x

space. The topology over H’p

(I)

is generated by the sequence of semlnorms

Ikl

k--O[9; p.

8].

A

sequence

1

in this space is said to converge to the element if

(4)

yk( @)

0 as for each k 0, i, 2, 3, A sequence

@9

in H

’p,8 (I)

Yk ( @n

is said to be a Cauchy sequence if

m )

0 as m, n independently of each other. It is a simple exercise to verify that the space Hv’p

(I)

is sequentially complete and so it is a

Frchet

space. Since

D(1)

c H’p

(I)

and the topology of

D(1)

is stronger than that induced on

D(1)

by H’p (I), it

,8

H,P

follows that the restriction of any f

(I)

to

D(1)

is in

D’ (I).

In view of the fact that

A

(xt) (-I

t F

(xt)

-P(x,t)

x where

k

-2i 2k-21

P(x,t)

tv+2p

ai

x+2P

t

i=l

ak being certain constants depending on and p, and the asymptotic orders [9, p.

B45]

(z)

o Izl" + Izl o

(5)

o Izl = zl (6)

where

max

( + 2p

2,

-) [8,

pp. 347,

351]

it follows that for fixed t

> O,

x

F

(ix) belongs to the space H

’p,8 (I)

when

treated as a function of x. Therefore, Hardy’s F -transform F(y) of a generalized

H,P

function f e

(I)

can be defined by ,8

F) =<f(x),

x F

(xy)>

y

>

0.

(7)

By following the technique as used in

[7]

it can be shown that F(y) is differ- entlable for each y

>

0 and that

F’(y) <f(x), {x F (xy)}> (8)

(5)

Note that

[x

F

(xy)]

also belongs to H’p

(I).

Y

We now state some results which will be used in the sequel.

Define

N

HN (t,)--

c (tx)

C (ylyay

o

N

[ x Cv+(xN)

C (iN) t C (iN) C

(xN)

-Q

(x,t)

2 2

h v+l

X t

where

Q (x,

t)

2 sin p sin (p

+ )

n

ff sin n

x t

(x

2 t

2)

x# t

(Io)

2 sin

p

sin (p+) L.

when t x

n sin 2

x

[8, p.

466].

Using the technique employed in proving Lemma 2 in

[7]

it can be proved H ,P

that for fixed t, x Q (x

t) (I).

It is now a simple exercise to prove for c

_> II, 8 _<

4 and

@ D(1)

that

b

x

Q(x,y) @ (y)

y dy also belongs to H’p

(I).

LEMMA 2. Let

k(t)

be defined as in section 2. Then for 0

<

y

< I

sup

0<t<

k ()

gk

(ty) =y

mln

(8 +

2, o 2k

k

O, I,

2,

PROOF. The result follows by dividing the t- llne into three parts 0

<

t

< I, I <

t

< l/y,

i/y

<

t

<

and considering the corresponding

sup 0<t<:

(6)

LEMMA 3.

Le__t

C

(z)

be the function

as

defined i_.p.n

(3)

and let

-%_< < %,

-v 2p

<_ <_ 3/2, 8 >

max

+

2p 2,

-1/2 ).

Then for flxed x

> O,

t F

(ty)

C

(xy)

ydy 0 in H’p

(I)

as 0

+

0

PROOF. The lemma can be proved by using lemma 2 and a variation of the technique used in proving lemma 4 of

LEMMA 4. Let

,

8, and p be restricted as in Lemma 3 and let H ,P then

,8

N N

< f(t),

t F (ty)

>

C (xy) ydy-

< f(t),

t F (ty) C

(xy)

ydy

>.

0 0

PROOF. The result follows in view of Lemma 3. The details of the technique to be used can be found in [7, Lemma

5].

LEMMA 5.

Le_.t

b

>

a

>

0

and (t,x),

Q

(t,x) b_e th__e

functions

a_.s

defined by

(9) and

(i0).

Then

llm b

..H (t,x)+

Q

(t,x)

xdx

a

I

t e

a,b]

0 t

4 [a,b].

PROOF. See Leuna 6 in

7].

LEMMA 6. Let the support of

D(1)

be contained in

(a,b)

where

b

>

a

>

0. Let

(t,x),

Q

(t,x)

be the functions as defined in

(9)

and (i0).

Assume that

- <_

v

< 1/2,

max

(-

2p,

v) _< < 3/2

and

_>

max

(v +

2p 2,

-1/2).

Then b

(7)

PROOF. The proof can be given only by using Lemma 3 and a simple variations of the techniques used in proving [7, Lemma

7]

and so the details are omitted.

3. INVERSION OF THE DISTRIBUTIONAL

F transform: We now state and prove our main result.

THEOREM. Let

-% <_ 1/2,

max

(-9

2p,

Iv l) <_ 3/2

and

8 _>

max

( +

2p 2,

-1/2).

H%)’P

Assume

that

F(y)

is the. distributional F -transform of f

(I)

as defined by

(7).

Then

F(y)

C

(x,y)

y dy,

# (x) <

f,

>

for each

@ D(1).

N 0

PROOF.

Let the support of

@

be

[a,b]

where b

>

a

>

0.

Since F(y) C

(xy)

y generates a regular distribution we have

N /

%)

\ b N

<F(y) C%)

(xy)y dy,

(x) (x)dx F(y)C%)(xy)

y dy

0 \ / a 0

--

a

(t), (t),

tt

(t,x)

0 F (ty)

+

C

QN(t’x) (xy) [7,

yLenadLemma

@ 4] (x) 8]

dx

(x)

dx

2 (t),

t

(t,x) + q(t,x) 9 (x)

dx

for N

>

b

>

0 [I, Lenna p.

394]

(8)

(t), ( x) +Q(

x x dx

by Riemann Sums technique 9, p.

148]

Lemma

6]

This completes the proof of the theorem.

Taking p 0 and p

1/2

in the above theorem we derive COROLLARY

I.

t f H

v’0

,8

(I1 where "%<- <- %’ )l <- <- 3/a

and

8 _> "%-

Define

th.._e

distributional Hankel transform of f by

F(y) <f(t),

t J

(ty)>

then

F(y) y j

(xy)

dy,

(x

N 0

fo__y_r al__l D(I).

COROLLARY 2. Let f H

’% (I)

where

"% <

9

< % II < < 3/2

and

8 _> "1/2.

Define

th__e

distributional

.Struve tr,ansform (H -transform)

of f by

F(y) <f(t),

t

Hv (t-y)>

then lira

fo__r al.._l D(I).

(9)

A.KNOW.LEDGMEN.T.

This work was supported by National Research Council Grant No. A5298. The first author is thankful to the Banaras Hindu University for granting him study leave.

REFERENCES

I. Cooke, R.G. The nversion formulae of Hardy and Titchmarsh, Proc. London Math.

Soc. 24

(1925)

381-420,

2. Erdelyi, A. (Editor)

Higher Transcendental Functi0.ns,

Vol. II, McGraw-Hill Book Co., Inc., New York, 1953.

3. Erdelyi, A. (Editor) Tables of Integral Transforms, Vol. II, McGraw-Hill Book Co., Inc., New York, 1954.

4. Hardy, G.H. Some ormulae in the theory of Bessel functions, Proc. London

Math.

Soc.

(2), 23,(1925)

ixi-lxlii.

5. Pandey, J.N. and Zemanian, A.H. Complex inversion for the generalized convolution transformation, Pacific J. Math. 25,

(1968)

147-157.

6. Pandey, J.N. An extension of Haimo’s form of Hankel convolutions, Pacific

J.

Math. 28

(1969)

641-651.

7. Pathak, R.S. and Pandey, J.N. A distributional Hardy transformation,

Proc.

Camb.. Phil...S0c.

76

(1974)

247-262.

8. Watson, G.N.

.A. treatise

on the

theory

of Bessel

funct.lons,

Cambridge University Press, 2nd edition, 1962.

9. Zemanian, A.H. Generalized integral transformations, Intersclence Publishers, 1968.

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