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On the factorization of certain probability distributions By HARALD CRAM~R

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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 i n r 7 ~ ...

R e a d 9 F e b r u a r y 1 9 4 9

On the factorization of certain probability distributions

By HARALD CRAM~R

1. The object of this Note is to show t h a t a large class of probability distributions of the type known as infinitely divisible have divisors which are not infinitely divisible. Among these distributions are, in particular, the Pearson Type I I I distribution and all non-normal stable distributions.

In the first two paragraphs, we briefly recall some known definitions and results. The main theorem will then be stated and proved in paragraph 3.

If ~ is a random variable, the probability of the relation ~= =< x is a func- tion

F(x)

of the real variable x. The function

F(x).

which determines the

probability distribution

of the variable ~:, is known as the

distribution /unction

(d.f.) of ~:. In order t h a t a given function

F(x)

should be the d.f. of some random variable, it is necessary and sufficient that F (x) should be never de- creasing and everywhere continuous to the right, and such t h a t F ( - - c ~ ) - - 0 and F ( + c ~ ) = l . The function

= f e"x d F

(t) (~)

~v

- - o o

is called the

characteristic /unction (c.

f.) of the distribution. To every d.f.

F(x),

there is one and only one c.f. ~(t), uniquely defined for all real t.

Suppose now that the variables ~=t and $2 are independent in the ordinary probability sense, and consider the sum ~: ~ ~:t + ~e. Let the d.f:s of the variables $, ~1 and ~2 be F, F1 and Fe, while the corresponding c.f:s are

~, ~1 and F2. We then have

F (x) : .t' $'~- (x ~- t) d F~ (t) = f F2 (x - - t) d F 1 (t).

- - o r - - o o

We shall say that F is

composed

of F 1 and

F2,

and use the abbreviated notation F = = F 1 * F 2 = F ~ F 1 .

To this symbolic multiplication of the d. f:s corresponds a real multiplication of the c. f:s. We have, in fact, $(t)--~ ~1 (t)q~2 (t). The operation of composition is commutative and associative, so that any symbolic product F ~ Ft ~ ' " ~ Fn is uniquely defined and independent of the order of the factors. The symbolic product of n identical factors will be written as a symbolic nth power: F In].

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H A r t A L D CP,~-M~R, On the factorization o f certain probability distributions

Thus the class of all d. f:s forms a semigroup with respect to the operation of composition. The u n i t element of this semigroup is the d.f.

l 0 for x < 0 , E ( x ) = ~ l for x_>-0,

which is the d.f. of a ~variable~> ~ which always takes the value 0. The only divisors of the unit are the d.f:s of the form E ( x - - m ) , where m is a con- stant. We have, in f a c t E ( x ) = E ( x - - m) ~ E (x ~ m). The corresponding rela- tion between the c. f:s is 1 = e " " . e - m u .

A ]actorization of the probability distribution defined b y F (x) is a n y repre- sentation F = F1 . . . F,,, where n > 1, and no Fr is a divisor of the unit.

Each Fr is then said to be a divisor of F. When F has no factorization, it is called indecomposable. A simple case of an indecomposable d . f . is

F ( x ) : p E ( x ) + q E ( x - - 1), where p and q are positive constants such t h a t p + q = 1.

2. The probability distribution defined b y F ( x ) is called i n / i n i t e l y divisible, if to every n ~ l , 2 . . . . we can find a d . f . G such t h a t F = G [''1. The pro- perties of infinitely divisible distributions have been studied by several authors, notably b y PAUL L~VY, who has shown (cf e.g. 3) t h a t the logarithm of the c.f. ~v(t) of a n y infinitely divisible distribution can be written in the form

(1) log q~ (t) ~-- m i t - - 89 a 2 t 2 -4- e itx - - 1 1 + x 2

- - o r

where m and a 2 > 0 are real constants, while M ( x ) i s real and never de- creasing in each of the intervals ( - - c ~ O) and (0, + c~), and such t h a t

1

M ( - - cx~) = M ( + cx~) = O, f x 2 d M ( x ) < c~. Further, a n y choice of m, a and

- - 1

M (x) consistent with these conditions yields an infinitely divisible distribution, and the representation of log ~(t) in the form (1) is unique.

The class of infinitely divisible distributions includes m a n y i m p o r t a n t types of distributions occurring in various applications. Thus for M ( x ) = 0 we have the normal distribution, and for a = O, M ( x ) = 2 E ( x - - 1) - - h E ( x ) the Poisson distribution. For a = O, M ( x ) = 0 for x < 0 and M ' ( x ) = ~ x - l e - a x for x > 0, we obtain the Pearson T y p e I I I distribution, and finally for a ~ 0, M ' ( x ) = A [ x ] -~-1 for x < 0 and M ' ( x ) ~ - B x -~ l f o r x > 0 , w h e r e 0 < a < 2 , we obtain the non-normal stable distributions.

I t follows from the above t h a t the problem of finding all possible factoriza- tions of an infinitely divisible d.f. F can be completely solved, as long as we restrict ourselves to factors which are themselves infinitely divisible. In fact, if F ~ F 1 ~ . . . ~ F,,, where every Fr is infinitely divisible, the logarithm of the c.f. ~vr corresponding to -Fr c a n be written in the form (1), and we must have m = ,.~ mr, a 2 =/,X~ ar, M ( x ) = ~ , M r (x). Converselv,~ anvo choice of the mr,

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ARKIV FOR MATEMATIK. B d 1 nr 7

~r and M r ( x ) consistent with these conditions yields a factorization of F, such t h a t all the factors are infinitely divisible.

In the two particular cases of the normal and the Poisson distributions, it is known (CRAM~R, 1, p. 52, and RAIKOV, 5) t h a t the faetorizations obtained in this way remain the only possible ones, even if we remove the restriction t h a t the factors F r should be infinitely divisible. Thus any divisor of a normal distribution is itself normal, and similarly for the Poisson distribution.

On the other hand, it has been shown b y examples (cf e.g. L ~ v G 3 and 4) t h a t there exist in/initely divisible d . / : s F such that F can be ]actorized into F - ~ F 1 * F2, where at least one o/ the ]actors is not in]initely divisible. This case occurs e.g. when F is the symbolic product of a certain number of ap- propriately chosen Poisson distributions.

The object of this Note is to show that, in fact, this property holds for a large class of infinitely divisible distributions.

3. Consider an infinitely divisible d . f . F, and let the logarithm of the corresponding c.f. ~ be represented in the form (1). The function M(x), being never decreasing, has almost everywhere a finite derivative M ' (x)> 0. We now proceed to prove the following theorem:

Suppose that We can ]ind two positive constants k and c such that M ' (x) > k ahnost everywhere in at least one o/ the two intervals ( - - c , O) and (0, c). T h e n F has a divisor which is not infinitely divisible.

Thus in particular the Type I I I distribution, as well as any non-normal stable distribution, has a divisor which is not infinitely divisible.

In order to prove the theorem, we may restrict ourselves to the case when the condition is satisfied in the interval (0, c). I t then follows from the pre- ceding paragraph t h a t F has an infinitely divisible divisor G defined by taking in the expression (]) of the c.f. m - - ~ a = - 0 , M ' ( x ) = - k for O < x < c , and M' ( x ) = 0 elsewhere. Thus we have only to show that G has a non-infinitely divisible divisor.

Denoting by y ( t ) t h e c.f. corresponding to G, we have according to (1)

c

(2) log ~2 (t) = k . e itx - - 1 1 + x 2] d x -~ log Yl (t) + log Y2 (t,),

0

where we take

i C

(3) log ~r (t) ~ - ~ e itx - - 1 ar (X) d x , (r =- 1, 2),

0

- - e for ( 8 9 1 8 9 + e)c, a I ( x ) = / 1 elsewhere in (0, c),

t

0 outside (0, c),

[ l + e f o r (89 e < x < ( ~ + e ) c ,

(4) a2 (x) = [ 0 elsewhere.

Here e denotes a constant such that 0 < e < 89

63

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ItAI1ALD CRAMI~R, On the factorization of certain probability distributions

It follows from (1) that y2(t) is the c . f . of an infinitely divisible d . f . G2.

We shall now show that, if e is sufficiently small, Yl (t) will be the c . f . of a non-infinitely divisible d . f . G1. Then by (2) we have G = G1 ~ G2, and our theorem will be proved.

For every real x, we define the functions fla (x), /32 (x) . . . . by writing fll (X) = ~ a 1 (x),

x

fl~ (x) = f 131 (x - - t) fll (t) d t,

0

fl,,

(x) = .t'~"-~ (x - t) ~ (t) dr.

0

We t h e n have ft, (x) = 0 everywhere outside (0, n c), and it is well known t h a t

w e h a v e

~ c c

f dtzfl,,(x)dx = k" ( r e ~.x al(z)dx)'.

0 0

Further, [fl,(x)[ < k"c '~-~ for all x, and it follows that

o o i i c c

1 ' ~ " ='s ~" . e~tZfl,~(x)dx--exp k. --1.

0 0 0

Writing

i i

: } c . % ( x ) dx, . . . 2 = k 1 + x X 2 ( 2 1 (X,) d ~ , ,

o o

we n o w o b t a i n f r o m (3) a n d (5)

w h e r e

( i ) ;

y l ( / ) - - e z..,it 1 +

eitZ 7fi! d;v = eitXdal(x),

0 - - z c

{

z

(;t (x) = e -~ E (x + ;~) + ~ n! l"

.--c.r

O b v i o u s l y G 1 ( - - c~) = 0, w h i l e f r o m (3) we o b t a i n (;l ( + co) ~= 71(0) -= 1. I n o r d e r t o p r o v e t.haf G l(x) is a d . f . , we now only h a v e t o s h o w t.hat it is n e v e r d e c r e a s i n g , i . e . t h a t ~ f i , ~ ( x ) / n ' > 0 for all x.

l

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ARKIV FOR MATEMATIK, B d 1 n r 7

Consider first 81@), which is everywhere non-negative, except between the limits (89 • e) c, where it takes the value - - k e. Further, as e ~ 0, it is obvious t h a t

fl2(x)

tends to k 2 ( c - - I c - - x 1) uniformly in 0 < x < 2c. Also it is easily seen t h a t for all sufficiently small e we have f12 (x) > 0 and f13 (x) > 0 for all x.

I t follows t h a t we can find eo such t h a t for e = Eo and for all x

fll(x) + ~.fi2(x) + l~.fia(x) >= O,

fl~

(x) = f 8~. (x - t) 82 (t) dt >: o,

0 3:

85 (x) -~ f 8a (x -- t) 82 (t) d t > 0

o

and hence ~ 8''~-(x-) > 0. Thus G1 is a d.f.

n! =

1

I t now only remains to show t h a t G1 is not infinitely

divisible.

I n fact, if G1 were infinitely divisible, log

yl(t)

could be expressed in the form (1) with a never decreasing

M(x).

Now since the derivative

M' (x)

exists almost every- where and is => 0, and since the representation (1) is unique, it follows from (2) and (3) t h a t we should have almost everywhere in (0, c)

k = M ' (x) + k a2 (x) > k a~ (x),

but this is obviously inconsistent with (4). Thus Gx cannot be infinitely divisible, and our theorem is proved.

4. By a theorem dt, e to KHINTCHINE (2), a n y d . f . which is not infinitely divisible has an indecomposable divisor. Writing the function G of the pre- ceding paragraph in the form G ~ G ['~1 ~- G ['~1 ~ ..., and applying first the argu- ment of the preceding paragraph and then KHINTCHINE~S theorem to each factor, we obtain the fol!owing result:

Any in/mitely divisible d. /. F satis/ying the conditions o/ the preceding theorem is divisible by the product o/ an in/inite sequence o~ indecomposable d./.'s.

R E F E R E N C E ~ : 1. C r a m ~ r , H . , R a n d o m v a r i a b l e s a n d p r o b a b i l i t y d i s t r i b u t i o n s . Cam- bridge T r a c t s in M a t h e m a t i c s . C a m b r i d g e 1937. - - 2. K h i n t c h i n e , A . , C o n t r i b u t i o n l ' a r i t h m 6 t i q u e des lois de d i s t r i b u t i o n . B u l l Math. Univ. Moscou. 1 (1937), p. 6. - - 3. L 4 v y , P . , Th6orie de ] ' a d d i t i o n des v a r i a b l e s al6atoires. P a r i s 1937. - - 4. - - - - , L ' a r i t h - m d t i q u e des lois de probabilit6s. J o u r n . Math. P u r e s et Appl., 17 (1938), p. 17. - - 5. R a i k o v , D . , On t h e c o m p o s i t i o n of Poisson laws. C. R. Acad. Scient. U R S S , 14 (1937), p. 9.

Tryckt den 19 april 1949

Upl)sala 1949. Ahnqvist & Wikse~ls Boktryckeri AB

65

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