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A R K I V F O R M A T E M A T I K B a n d 1 nr 8

C o m m u n i c a t e d 1 2 J a n u a r y 1 9 4 9 b y I-I. C R A M ~ R

S t o c h a s t i c p r o c e s s e s a n d i n t e g r a l e q u a t i o n s B y U L F G R E N A ~ D E R

1. I n the following we shall consider stochastic processes, i.e. real functions x (t, o~) of the two a r g u m e n t s t a n d o~. t will denote a real p a r a m e t e r in a finite or infinite interval T. (o will be a, point in a n a b s t r a c t space 52, on which is defined a m e a s u r e of p r o b a b i l i t y in the usual way. F o r fixed t E T, x (t, @ is supposed to be m e a s u r a b l e in 52 a n d t h e following integrals existing

i r a ( t ) = f x ( t , eo) g P ( ( o ) .... E x ( t )

o

i ~ (s,

t) = R [ . (,) - .~ (s)] [x (t) - ~ (t)].

Moreover, we suppose t h a t x(t) is continuous in the m e a n , i.e.

E [ . (t + h) - x (t)] 2 -~ 0

for e v e r y t as /~,-> 0. L e t T == (a, b)! Suppose t h a t we know r (.~, g) and t h a t m (t) is an u n k n o w n c o n s t a n t = m, which is to be estimated. U n d e r certain as- s u m p t i o n s it can be shown t h a t one is led to consider estimates of the form

b

,,,,* = .(.~: ( t ) / ( t ) ~I t,

where / ( t ) is q u a d r a t i c a l l y integrable and the integral is t a k e n in the sense of K a r h u n e n (l~:ber lineare M~:thoden in der Wahrschein]ichkeitsrechnung, Ann Ac Sol Fenn, series A, I, 37, Helsinki 1947). To determine the best e s t i m a t e of this f o r m we d e m a n d t h a t ,,,* will 1)e unbiased a n d of m i n i m u m variance, i. e.

But this implies

I

]5' ?~,~: =.- %q.

t ~: [',,c '~ - -- m]" - ~, ,." , .

I

,/:l ( n <i t -= I

h b

I =

.f (r

(.. t) / (,~) / (t) #,~ g t = . , 2: ,,..

- a a

7 67

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U. GRENAI",IDER, Stochastic processes and integral equations

As J'J'r (s, t) [ (s) / (t) d s d t =: E [ f [x (t) - - m (t)] / (t) d t] ~ >-- O, the kernel r (s, t) has positive eigen-values, so that we can apply the theorem of Mercer and obtain

r(s, t) = ~ %(s)(p,(t) A.~ 1 2 ,

with the characteristic elements 2 and ~ to the integral equation qJ(s) = 2 f r(s, t ) ~ ( t ) d t .

Putting a, = f q~ (t) dt and c,. = .l'/(t) % (t) d t we get the conditions

~ , c , . a , = l , \~ c~ < cxz "9 c; = r a i n .

1 1 I )~r

In order to get convergent series we must separate several cases.

only the main result obtained by applying the Schwarz inequality:

The estimates

b

m o _ 1 n = l .

~_~ "

1

satis/y the relations

E m n ~ m ; ~. E [ m ~ - - m ] ~ ~ G . L . B . I as n ~ co.

We state

When m* converges in the mean, its limit is unbiased and o~ minimum variance.

2. There are obvious generalizations of the above. But to treat the general problem of unbiased estimation we must use another method. -(2 m a y be an N-dimensional Euclidean space, corresponding to an N-dimensional stochastic variable, or it m a y be some appropriate subset of all real functions, corre- sponding to a stochastic process. On ~ is defined a measure of probability P (w, 0) depending upon a real parameter 0, a ~ 0 ~ b. To each 0 corresponds the Hilbert space L2 (Q, 0) of quadratically integrable functions with respect to Po and with the usual quadratic metric.

Consider the operation

T o g = .fg(o))dP(~o,O); gEL2(D,O).

Let the following conditions be satisfied:

A L2 (~2,0) shall be the same for all 0 (consisting of the same elements, but usually with different metric) and the topological structure shall be in-

dependent of 0.

B T,, shall transform L2 (/2) into L2 (0; a, b).

C The functionals To shall be of uniformly bounded norm [ T o g [ ~ K . g o ~ , ; a ~ O ~ b . 68

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ARKIV F6R MATEMATIK. B d 1 nr 8

I t is possible to show t h a t for the validity of A--C the following simpler condi- tions are sufficient. Let

I : { a i ~ x ( t ) ~ b i ; i = 1 , 2 . . . . nl

be an arbitrary finite-dimensional interval and demand that for every I a. P (I, 0) shall be continuous in O.

b. P (I, 0') <_ C. P (I, ~") for every O" and 0".

Under the assumptions A--C it can be proved, using an important theorem of Hilbert concerning completely continuous infinite quadratic forms that there exist two ortho-normal systems {YJ, (r and I~, (e))} and a sequence of numbers

{),,. } so t h a t

~f~ (0) = 2, f ~, (o9) d P (w, 0).

22

Now again we must distinguish between various cases. Let us suppose, e.g., t h a t {%} is complete! Then the following theorem is easily obtained:

T h e o r e m I. Under the said canditions it is necessary and su//icient /or the exist- ence o/ an unbiased estimate O"E L2 (~2) o/ 0 that

b

~,2~,c~ < ~ where c,.= f ~w,.(O)dO.

i]

This is, of course, connected with the theorem of Picard for usual integral equations.

3. We shall now treat a different problem with similar methods. Let a be a bounded measure on the real axis, and x(t) a stochastic process with t r (s, t) ] < K. Then s t u d ~ n g the integral equation

z ( e o ) = ~ J x(t)/(t)d(~(t); z e L 2 ( x ) ; / e L e ( a )

it is easy to show that the process can be represented as

. r ( t ) = z, - - - ,

, V L

where both z, and ~ are obtained as eigen-functions to symmetric integral equtltions. This is only a simple generalization of a result due to Karhunen.

(Zur Spektraltheorie stoehastischer Prozesse, Ann Ac Sci Fenn, series A, I, 34, Helsinki 1946.) But for an orthogonal process Z(4) with : I Z ( 4 ) 2 ~ ~(4), one can prove, using Parsevals relation and the defiping properties of an orthogonal process:

69

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U. GRENANDER, Stochastic processes and integral equations T h e o r e m II.

Z

z(;.)=

~,,.

where {z~} is a CON system in L 2 (Z) and {q),,} is a CON system in L2(a ).

Applying this to the above one gets

T h e o r e m III. The process can be represented as

o r

x (t) =

./1

(t, ;,) d Z

(~)

,where /or every t /(t, 2)E Le (a) as a /unction o/ )~ and Z (),) is an o,rthogonal process with [~ Z (~)!2 = a (~).

Detailed proofs and various further developments o f - t h e methods used here will be reserved for a later publication.

[['rs'ekt~ d e n tl m a j ig,I!)

70

UlmRal,q 1949. Almqvi~t & \VikseUs Y~oldry('keri A B

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