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On the field of operators of Ditkin and Prudnikov

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ANNALES SOCIETATIS MATHEMATICAE POLONAE Series I : COMMENTATIONES MATHEMATICAE X I I I (1969)

В. P. P arashar (Mandla)

On the field of operators of Ditkin and Prudnikov

1. Introduction. An operational calculus for the operator — 2—

has been developed by Ditkin and Prudnikov [1] on the lines as Miku- siński [2] has done for the operator d/dt. The procedure of Ditkin and Prudnikov is as follows:

Let L be the set of all locally integrable functions existing on the half-line 0 < t < oo and vanishing on the left-half of the real line and also satisfying the condition, J -— J \f(t)\dt< oo for any t0 > 0. M

о £ о

t I

denotes the set of all functions of the form J — § f{t)dt-\-C, where f(t)e L and C is a constant. M then forms a commutative algebra without zero divisors, with sums and scalar products defined in the usual way and product defined as,

t i

f ^ Y g l i ł — riW—ęyidri-,

о

0

M is then extended to a quotient field.

In what follows, we shall define product in M as,

t i

Ц.1) f-g(t) = J d f J / ( 4 J)S[ ( l - 4) ( « - f ) ] * ,

0 0

and denote the quotient field thus obtained by m.

The object of this note is to study some analytic and algebraic prop­

erties of m.

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58 В. Р. P a r a s h a r

2. If h denotes the Heaviside’s unitary function, then,

( 2 . 1 )

Thus h acts as an integral operator in this calculus. The correspond­

ing differentiation operator is defined as, В = l[h (here 1 is the multi­

plicative identity of m). By induction we can prove that,

stant, f e L and g eM, we can imbed the set of numbers, L and M respectively in m.

d d The following theorem gives a relation between В and — t— :

dt dt

T h e o r e m 1. Let feM possess a locally integrable derivative of order 2k) furthermore let us suppose the limits

(

2

.

2

)

B n {(w—-l)!}2

By the mappings a о a — , f о f — and g о g — , where a is a con-

h h h

to exist. Then

P roo f. By direct computation we see that,

i.e.

h Hence

The theorem can now be proved by induction.

Relation (2.3) reduces to,

(2 .4 )

(3)

for functions which are continuous in all their derivatives up to к —1.

In (2.3) a single discontinuity at t = 0 has been assumed but the gen­

eralization to the case of a finite number of discontinuities is not diffi­

cult.

T ra n s la tio n o p erato r. Let

Then

S x{t) = 1 °, u ,

0 < ź < A, 0 < A< t.

If we denote the operator d

(*-A ) d

by B x, then d(t — X) d (t— A)

B x{Hx(t)f} = f ( t —X). Thus f = B xH^(t) acts as the translation operator in this calculus.

3. L e m m a 1. I f f(t)eM and

K T = max {\f(t)\}, 0

then

IA *)I<- z f f 1 {(те—l ) ! } 2 P ro o f. The result is true for те = 1.

If it is true for те, then

L f + 1 («)l = ! / ” (*)! • 1 / ( 0 1

K 'r'1 ("

{(» —!)!}■

Ę + 1 { ( » - ! ) !}2

t 1

J d ( J r T - ' f - ' d r , =

0 0

K n T+1tn {n\}2

(3.1) C orollary . F or feM , f n> 0 as n -> oo uniformly for every interval 0 < t < T.

This is the analogue of a theorem of Ryll-Nardzewski [3] in the operational calculus • of Mikusiński.

From Lemma 1 and (3.1) we easily derive

O O

T h e o r e m 2. I f the radius o f convergence of the series an Xn, where

n= 0

« 0 , 0 ! , . . . are numerical coefficients and A a complex number, is positive.

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60 В. Р. P a r a s h a r

then the series £ anXnf n, /elf, regarded as a series of two variables A and t

»=i

is uniformly convergent in every domain 0 < A < A0, 0 < £ < .

The theorem has an analogue in the operational calculus of Miku- sinski.

4. Linear mappings. Let Mv = { f : where M* = M — {0}. Clearly

m = { J {M p}.

P tM *

We now derive the following results:

(i) Mp is a module over I f .

For if geMp, then g = fjp for /elf.

Hence rg = rf[p eMp, where r elf.

(ii) Mp is not an algebra over M.

For if Tc, leM p, then Tc = fjp , l = glp. Hence k-l = (1 lp)(fglp)- Since in general fg jp iM , in general Tc • 1 4 MP.

Provide a relation < to M* defined by c < d if there exists b e lf such that be — d. The relation < directs the set M.

(iii) I f p < g, then Mp a Mq.

For if xeM p, then x = f/p for /elf.

Since q — Jcp for some 1c elf, x =//p = TcflqeMq. Hence xeM q.

The mapping p -> Mp thus defines a net in {Mv}. Let D be the set d d

of fe M such that D is closed with respect to the operator — t— . dt dt Let S be the subalgebra of m defined by S = {aem : aD c f>} and N = {p e lf*: — -D c f>).

Let MN = P {Ifp]-

P<lN

The following results are now obtained:

(A) N is closed under multiplication.

For if p , q eJV, th en --- D — — (— • D 1 <= — D c= D. Hence pqeN .

p-q p \ q I p

(B) MN is an algebra over M.

For if x ,y e M Nl then x = f[p , y — — for p . q e N and f,g e M .

<1

Hence xy = fg[pqeM pa. Since pqeN , xyeM N.

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(C) M N C= 8 .

For if xeM x, then x — f[p for some p eN , feM . Hence x -B = — В f P

= /• c /Н cz B . Hence xeS.

The author is grateful to Dr. C .B .L . Verma for kind encouragement during the preparation of this note.

References

[1] D itk in and P ru d n ik o v , Integral transforms and operational calculus, 1965.

[2] J . M ik u siń sk i, Operational calculus, 1959.

[3] R y ll-N a r d z e w s k i, Sur les series de puissances dans le calcul operatoire, Studia

Math. 13 (1953), pp. 41-47.

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