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On a class of orthogonal series

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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 n r 2

C o m m u n i c a t e d October 27, 1948 b y F. CA~LSO~

On a class of orthogonal series

By H. BOrtMAN

1. L e t { ~ ( x ) } denote a normahzed orthogonal system, defined in the inter- val (a, b) and belonging to t h e class L 2. The famous theorem of RADEMACHER- MENCr~OFF [I: 162] tells us t h a t

~ an~n(x)

r ~ = l

is convergent almost everywhere in (a, b) if a~ (log n) < c~.

Conversely, if X a ~ ( l o g n ) ~ : - c~ then it is possible to find a system {~v~} for which

.~anC, Vn

is divergent almost everywhere.

In order t h a t

o o

an<- c~

should be a sufficient condition for the convergence almost everywhere of the series it will thus be necessary to specialize the orthogonal system. KOLMOGOROI~F h a s found t h a t if {~v~} is a system of independent random variables, then

Xa~

< c~ is a necessary and sufficient condition for the convergence almost everywhere of the series. The object of the following paper is to generalize slightly this result of KOI,Moe~oRoFF.

2. I n dealing with questions of this kind, the theory of the torus space seems to be very useful. Following JESSEN, who made the first systematic study of this space, we denote it b y Q(.~.

Q~ is an w-dimensional vector space, consisting of all infinite sequences of real numbers ~ = (Xl, x2 . . . xn, . . . ) where 0 --< xn < 1 for n = 1, 2 . . . The subspace Qn consists of the points $~ = @1, x2 . . . x~). I n the same w a y Qn, co consists of the points $~, r = (Xn+I, X~+2, 9 . .). We m a y then consider Q~ as the product space Q~ = (Q~, Q., (,). I n accordance with this notation we m a y write

= (~., ~ , ~).

The following two theorems of J~SSEN are fundamental for the theory.

2 13

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If /(~) is an integrable function in Q(o then

(2.1) f t($)d$

Q~

and

(2.2)

1 1 1

= l i r a

f / ( ~ ) d $ ~ = l i m f d x n f d x n - l " " f ] ( $ ) d x 1

n ~ ZC Qn n ~ or 0 0 0

lim f ] ($) d ~., ~, = / (~) almost everywhere.

It ~ OO Qn, (o

3. I t is easily seen t h a t an enumerable set of independent random variables may be represented in Q(o as a system of real functions with the following property.

If /~ (~) for n - ~ 1, 2 . . . . denotes a random variable then

]n (~)~ ]~

(xn), i.e.

for each n /n(~) depends only on xn.

Having noticed this fact we can state KOLMOGOI~OFF'S theorem in the following

f o r m .

Let {~n(~)} denote a normalized orthogonal system in Q~., and suppose t h a t

~n(~) = ~.(x~) for each n [III: 14l]. Then the series

a n C f n ( X n ) n = ]

converges almost everywhere in

Q(,,

if L'a~ < c~ but diverges almost everywhere if

Z a~ = c~.

The first part of this theorem m a y be proved as follows.

By the RIESZ-FISCliER theorem the partial sums

N

Z ancfn(Xn)

n = l

converge in mean to a function ~0($).

By theorem (2.1) [II: 286]

N

f q)(~) d~,_v,,, ~-- ~.an~n(Xn)

QN, • n = l

and hence by theorem (2.2)

25

lira ~ an ~n (x~) = T (~) almost everywhere.

Well-known examples of orthogonal systems of this type are a) RADEMACHER'S system {rn($)}, [I: 42], where

rn($)~

b) The system {0~(~)}, [I: 134], where 0 n ( $ ) = e e'ix~.

{

+ 1 if 0 < x n < 8 9 0 if x n = 0 or 89 --1 if 1 < x ~ < 1

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.ARKIV FOR MATEMATIK. B d 1 n r 2

4. L e t {q. (x.)} be a normalized orthogonal system of the type just mentioned.

We will now define a new system of functions {W~(~)} in the following way.

Let

n = e l + e2 2 + e 3 2 2 q- . - -

b e the expression for n in the dyad scale. If e~ is 1 for v = v 1, v2 . . . . v~ and

0 otherwise, we denote b y Wn(~) the product q~- %,~" q,:, -.. %~.

B y virtue of FUBINI'S theorem

1 1 1

Qt,j 0 0 0

and hence {~v~(~)} is normalized. It is also orthogonal.

Q~o

For

may be expressed similarly as a product of integrals, one of which, at least, is of the form

1

f rfkdxk = O.

o

Starting for example with RADEMACHER'S system {r,J, [I: 132], we obtain a system {~}, which is easily identified with WALsu's system.

5. In this and the following sections we will deduce some theorems concerning real orthogonal systems of the type {yJn}.

5.1. We define the distribution function for a measurable function q(x) as F (t)= m E (q~(x) < t).

Suppose t h a t the distribution function of each q~ is continuous. Then ~an~fn iS either convergent almost everywhere or divergent almost everywhere.

To prove this theorem, w e make the following purely formal decomposition of the series

S = a n o n = a 2 n + l ~ 2 n + l q- " ~ a 2 n ~ 2 n ~--

n = l n = 0 n = l

= ~ I ( X l ) Z a2n+ l V, g2n q- a2n y)2n = Cfl " S1 -}- S 2

n=O n = l

where S 1 and $2 are independent of x 1.

15

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If S and $2 are convergent, then S1 is convergent. If S is convergent but

$2 divergent, then S 1 is divergent. If a and fl were two different values of ~01 for which the latter case would occur, then ( a - fl)S1 would be convergent, contrary to the hypothesis. Consequently, for e~ch ~ , ~ there is at most one such value a. According to our assumption the distribution function of ~01 is continuous; hence m E (9l = a) = 0.

We can therefore state: If S is convergent in a set E, both S1 and $2 are convergent almost everywhere in E. This may also be expressed in the following way: The measure of E is independent of x 1. Si and S2 are, however, orthogonal series of the same type as S. The argument m a y be applied once again; m E is independent of xz. We proceed in that way and obtain:

For each n, m E is independent of Xx, xz . . . . x.. By an important lemma of JESSEN m E is then either 0 or 1 [II: 270].

5.2. Consider again a system of the type {qn}.

As coefficients for the series we choose a system of functions {/,}, belonging to L 2 and with the property

/ n = / n ( X l , X 2 , . . . , X~-I) for every n.

Let S, for v = 1, 2 . . . . denote the partial sums and E,v the set where

then

bound {I S~ l, I $21 . . . I S,v l} > e

Z f/:d

~,=1 Q,.

r u e s < 8 2

To prove this, let Bn be the set where [Sn ] > e and B* the complementary set of B~. We m a y evidently write [II: 275, III: 141]

Eiv = B 1 + B~B~ + BaB~ B{ + ... + BN B ) - I B ) - 2 " " B { = A 1 + A2 + Aa + " + A s . According to our hypothesis An is for every n a cylinderset in Q,,, with its base in Qn.

A n A n An A n

Adding these relations for n = 1, 2 . . . N, we get

/V

The inequality is thus proved. The method of proof also gives the following extension.

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ARKIV FOR MATEMATIK. B d 1 n r 2

L e t q be a function of the variables

xlr x~e+2 .. . . only, i. e. g =

g(x~v+l, xs+2 . . . . )

and let Ely be the set where then

bound {[a&l, l a & l . . . . ,

mE:v< f g2d~=l Q~,

~2

5.3. We return to series of the t y p e ZTan ~vn and denote their partial sums b y r i . e .

zV

* = 0

I t is easily seen t h a t the subsequence a2n is convergent almost everywhere, if

Xa~ < co.

Since q2v converges in mean to a function a and f a d s =

Q iv , v~

we have b y JESSE~'S theorem (2.2)

lira %N = a almost everywhere.

6. We will now denote a function yJ b y ~0 (k) if it has k factors. We then divide the system {~n} iato partial systems

~)~ . . .

~ n ' k = l , 2, 3,

I n each partial system the indices of the functions are changed, while the mutual order is kept unaltered.

We can now deduce the following theorem.

If 2:a;~ < 0% then the series

~ an v2~)

n = l

is convergent almost everywhere for every k.

This can be proved by induction. F o r k = 1 the theorem holds true, and moreover we have the following inequality (cf. 5 . 2 )

N

m E

boundl~ :--~lv {[S('~/I} > e < ~ +=~

17

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Suppose t h a t the t h e o r e m holds for k and t h a t

m E tl~b~ {1 S(k),' 9 [} > k e < ~ z-. a,..

U n d e r these assumptions we can prove the t h e o r e m for k + 1.

B y using the same m e t h o d of proof as in 5.3 it is easily seen t h a t the se- o(k+l)

quence ~(k+~+O is convergent almost everywhere, when v runs t h r o u g h O, 1, 2, . . . and ,,(k+l+v)v ----(k+l)-lv,(k + l + v ) ,

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

F o r k + + v < n < k - 2 v the functions on - - o / k + l + < are of the form

v + k ,,, )

,,,_(k+xo+g

,Ikl

~k+24-. z/J atk+l+~ , " ~lt "

[t=l ( ~ ] ~-#

The upper bound for these \ v + functions is greater t h a n k e in a set E,,.

The characteristic function of E . is denoted by /(E,,) 1

m E , = f t(F ,)ae = f . d x k , + l §

Qr 0 (Qk+ 1+,', Qk+2-k',', (,~)

According to our assumptions the second integral is less t h a n

~,--1 J

;,,~=-~+,,+2 k \~ ..,

,~.~'J---- 1 a(k+l,+0+'~

and hence

]r \ ,+1 ] 1 ]C t ,.+l )

, . , r = -

t t = l /e=l

~-a m E~ is thus convergent; hence m [ ; = m lira sup E~ = O.

Choosing v(n) so t h a t

a}k+l+~,~,

t, ,, ) 7 - , ~

we get

(k + 1 + v(n)] (k + 2 + v ( n ) l v(n) ] < n - < v ( n ) + l ] [ '~k~-' 1) ~(k§ ]

lim sup - . ' --*~(k+x+,,<n)~ < k e almost everywhere.

n ~ oo k ~, (n) )

s is arbitrarily small, and hence

---- lira b'(k+~+,.~ almost everywhere.

l i r a S~ k+l) --(k+l)

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ARKIV FOR MATEMATIK. B d 1 n r 2

To prove the inequality for k + 1, observe that the above proof gives the following relation.

Let E1 be the set where

-- { k + l + r ( n ) ' ~ ~ > 8

bound { S~ k+l) S (k't'l}

1-<- n <-- N \ ',, (n) .) J

then

k s

m E 1 < ~ ~ a ~ .

Next we have

~,+1 7 S(k+l) o I k + l )

i. e. the sequence

s(k+l)

/k+x+~,'~, 'P : O, ] , 2 . . . . ,

is of the same type as the sequence S~, studied in 5.2.

Let v 0 be the smallest integer for which k +,2 + ro~

v 9 + l I > N and E 2 the set where

(k+l)

b o u n d S~+1+~, l} > e then, using theorem 5.2, we get

m E2 < --~ ~ . a; < a;.

* = 1 - - ~ , r = l

From these relations we obtain the desired result

m E {bound { I S n ' k + l ) l } > ( k + l ) ) < e--- ~ /~,a~.

- l ~ n ~ N ~=1

R E F E R E N C E S . [I] K a c z m a r z & S t e i n h a u s : T h e o r i e d e r O r t h o g o n a l r e i h e n . W a r s z a w a 1935. - - [II] J e s s e n : T h e t h e o r y of i n t e g r a t i o n i n a s p a c e of a n i n f i n i t e n u m b e r of d i m e n - sions. A c t a m a t h e m a t i c a 63 (1934). - - [ I I I ] L 6 v y : T h 6 o r i e d e l ' a d d i t i o n d e s v a r i a b l e s al6atoires. P a r i s 1937.

T r y c k t d e n 10 f e b r u a r i 1949.

Uppsala 1949. Almqvist & Wiksells Boktryckeri AB

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