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Vol. 24, No. 1 (2000) 29–42 S0161171200002945

© Hindawi Publishing Corp.

ON CONDITIONS FOR THE STRONG LAW OF LARGE NUMBERS IN GENERAL BANACH SPACES

ANNA KUCZMASZEWSKA and DOMINIK SZYNAL (Received 4 August 1998 and in revised form 26 March 1999)

Abstract.We give Chung-Teicher type conditions for the SLLN in general Banach spaces under the assumption that the weak law of large numbers holds. An example is provided showing that these conditions can hold when some earlier known conditions fail.

Keywords and phrases. Random element, Banach spaces, weak law of large numbers, strong law of large numbers.

2000 Mathematics Subject Classification. Primary 60F15, 60B12.

Let(,) be a real, separable Banach space. A strongly measurable mapping X from a probability space(Ω,,)intoᏮis said to be a random element.

IfEX<∞, then the expectationEXis defined by the Bochner integral.

Strong laws of large numbers (SLLN) for random elements, i.e.,(X1+···+Xn)/n→0 a.s.,n→ ∞, were investigated by Mourier [14], Fortet and Mourier [8], Beck [3], Beck and Giesy [4], Hoffman-Jørgensen and Pisier [10], Heinkel [9], Taylor [17], Woyczy´nski [19], and Adler, Rosalsky, and Taylor [1]. Their efforts have concentrated on a complete characterization of all those Banach spaces in which the SLLN holds under condi- tions of classical probability theory or on finding conditions on the random elements which ensure the SLLN. It is known (Woyczy´nski [19]) that in certain Banach spaces the Chung’s condition (Chung [7]) implies the SLLN for a sequence of independent random elements.

Some handy conditions for the SLLN in Banach spaces were given by Kuelbs and Zinn [13] and by Alt [2].

Extensions of the Chung-Teicher type conditions (cf. Chung [7], Teicher [18], Chow and Teicher [6]) for the SLLN for sequences of independent random elements in Hilbert space were found by Szynal and Kuczmaszewska [16], Choi and Sung [5], and Sung [15].

The aim of our paper is to give conditions for the SLLN in Banach spaces which can be applied in more general cases than those of Choi and Sung [5], Sung [15], Adler, Rosalsky, and Taylor [1] and Kuczmaszewska and Szynal [12]. We present also an example showing that these conditions can be applied when some earlier known conditions fail. We make use of the following lemmas.

Lemma1(cf. Yurinskii [20]). LetX1,X2,...,Xnbe independent-valued random el- ements withEXi<∞, i=1,2,...,n. LetᏲkbeσ-field generated by(X1,X2,...,Xk), k=1,2,...,nand let0= {Ω,∅}. Then for1≤k≤n,

ESn|k

−ESn|k−1≤Xk+EXk, whereSn= n i=1

Xi. (1)

(2)

Lemma2(cf. Choi and Sung [5]). Let{Xn, n≥1}be a sequence of independent,- valued random elements. Then

Sn

n →0 a.s.,n → ∞ (2)

if and only if S2k

2k →0 a.s.,k → ∞ and Sn

n

P 0, n → ∞. (3)

Let a functionφ:RR+be nonnegative, even, continuous and nondecreasing on (0,∞)with limx→∞φ(x)= ∞and such that

(a) φ(x)/xor (b) φ(x)/x,

andφ(x)/xp,x→ ∞,for somep, 1< p≤2.

Theorem3. Let {Xn, n 1} be a sequence of independent-valued random elements. Suppose that in the case (a) for somep, 1< p≤2,

(A)

j=2j−pE φpXj

φp(j)+φpXjj−1

i=1ipE φpXi

φp(i)+φpXi<∞, (B) n−pn

i=1ipE φpXi

φp(i)+φpXi=o(1), (C)

n=1P(Xn ≥an) <∞,

for some sequence{an, n≥1}of positive numbers such that (D)

n=1φp(an)E φpXn

φ2p(n)+φ2pXn<∞ or in the case (b) for somep, 1< p≤2,

(A1)

j=2j−pE φXj

φ(j)+φXjj−1

i=1ipE φXi

φ(i)+φXi<∞, (B1) n−pn

i=1ipE φXi

φ(i)+φXi=o(1),

and (C) is satisfied for some sequence{an, n≥1}of positive numbers such that (D1)

n=1φ(an)E φXn

φ2(n)+φ2Xn<∞.

Then

n−1 n k=1

Xk−EXk P

0, n → ∞, (4) if and only if

n−1 n k=1

Xk−EXk

→0 a.s.,n → ∞, (5)

whereXk=XkI[Xk ≤k].

Proof. Suppose that (4) holds.

Letr≥1. We note that

n=1

P

XnXn

= n=1

E

IXn≥n

·IXn≥an

+IXn≥n

·IXn< an

n=1

PXn≥an +2

n=1

E φ2rXn

φ2r(n)+φ2rXnIXn< an (6)

(3)

n=1

PXn≥an +2

n=1

φr(an)E φrXn

φ2r(n)+φ2rXn<∞, where we putr=pin the case (a) andr=1 in the case (b).

Hence{Xn, n≥1}and{Xn, n≥1}are equivalent. Therefore, by (4), we have

n−1

n i=1

Xi−EXi

P 0, n → ∞. (7)

Write

Xk=Xk−EXk, k≥1, Sn= n k=1

Xk, Sn= n k=1

Xk. (8)

Define

Yn,i=ESn|i

−ESn|i−1

, (9)

whereᏲi=σ (X1,X2,...,Xi)andᏲ0= {Ω,∅}.

Note that{Yn,i,1≤i≤n}is a martingale difference for fixedn. Then we have Sn−ESn=

n i=1

Yn,i. (10)

Now we prove thatESn/n→0, n→ ∞. Using (9) and Lemma 1, we get PSn−ESn> nε

≤ε−2n−2ESn−ESn2

−2n−2E n i=1

Yn,i

2

−2n−2 n i=1

E Yn,i2

≤ε−2n−2 n i=1

EXi+EXi2

−2n−2n

i=1

EXi2−2n−pn

i=1

ipEXip ip .

(11)

Hence in the case (a) by (B), we get PSn−ESn> nε

16ε−2n−pn

i=1

ipE φpXi

φp(i)+φpXi=o(1), (12) while in the case (b) by (B1)

PSn−ESn> nε

16ε−2n−p n i=1

ipE φXi

φ(i)+φXi=o(1). (13) Therefore, in the case (a) and (b) we have

n−1Sn−ESnP 0, n → ∞. (14)

(4)

Thus we conclude, fromSn/n P 0, n→ ∞, and (14), that ESn

n →0, n→ ∞. (15)

Now we are going to prove thatSn/n→0 a.s.,n→ ∞. By Lemma 2 it is enough to prove thatS2k/2k0 a.s.,k→ ∞or equivalently, asES2k/2k0, k→ ∞, that

2−kS2k−ES2k →0 a.s.,k → ∞. (16) Taking into account the identity

Sn−ESn2= n i=1

Yn,i2 +2 n i=2

Yn,i i−1

j=1

Yn,j, (17)

we see that

2−2nS2n−ES2n2=2−2n

2n

i=1

Y22n,i+2

2n

i=2

Y2n,i i−1

j=1

Y2n,j

. (18)

Now, put

Z2n,i=Y22n,iIXi< ai

−E

Y22n,iIXi< ai

|i−1

, 1≤i≤2n. (19) Then by Chebyshev’s inequality, equation (9) and Lemma 1, we have

n=1

P

2n

i=1

Z2n,i

> ε22n

≤ε−2 n=1

2−4nE

2n

i=1

Z2n,i

2

−2 n=1

2−4n

2n

i=1

E

Y24n,iIXi< ai

≤ε−2 n=1

2−4n

2n

i=1

EXi+EXi4IXi< ai

≤ε−228 n=1

2−4n

2n

i=1

EXi4IXi< ai

≤ε−2 212

15

i=1

i−4EXi4IXi< ai .

(20)

Hence we see that in the case (a) under the assumptions (C) and (D) we have

n=1

P

2n

i=1

Z2ni

> ε22n

≤ε−2 212

15

i=1

i−2pEXi2pIXi< ai

≤ε 212

15

i=1

2pXi

φ2p(i) IXi< ai

≤ε−2213 15

i=1

φp(ai)E φpXi

φ2p(i)+φ2pXi<∞.

(21)

(5)

Similarly, in the case (b) under the assumptions (C) and (D1) we lead to

n=1

P

2n

i=1

Z2n,i

> ε22n

≤ε−2 212

15

i=1

i−2pEXi2pIXi< ai

≤ε−2 213

15

i=1

φ ai

E φXi

φ2(i)+φ2Xi<∞.

(22)

Therefore, by the Borel-Cantelli lemma, we state that

(2n)−2 2n

i=1

Y22n,iIXi< ai

2n

i=1

E

Y22n,iIXi< ai

|i−1

→0 a.s.,n → ∞.

(23) Now, note that in the case (a) the assumption (B) implies

2n−22n i=1

E

Y22n,iIXi< ai

|i−1

2n−22n

i=1

EXi+EXi28

2n−22n

i=1

EXi2

16

2n−p2n i=1

ipE φpXi

φp(i)+φpXi=o(1).

(24)

Similarly, in the case (b), by B1, we get 2n−22n

i=1

E

Y22n,iIXi< ai

|i−1

16

2n−p2n

i=1

ipE φXi

φ(i)+φXi=o(1). (25) Therefore, in the case (a) and (b), we obtain

2n−22n i=1

Y22n,iIXi< ai

→0 a.s.,n → ∞. (26)

Using the assumption (C), we get 2n−22n

i=1

Y22n,iIXi≥ai

→0 a.s.,n → ∞ (27)

which proves in the end that 2n−22n

i=1

Y22n,i →0 a.s.,n→ ∞. (28)

Now we see that

Yn,ii−1

j=1Yn,j, 2≤i≤n

is a martingale difference for fixedn.

Therefore, in the case (a), after using Chebyshev’s inequality, (9), and Lemma 1,

(6)

we get n=1

P

 2−2n

2n

i=2

Y2n,i i−1

j=1

Y2n,j

> ε

≤ε−2

n=1

2−4n2 n i=2

E Y2n,i i−1

j=1

Y2n,j

2

≤ε−2 n=1

2−4n

2n

i=2

E Xi+EXi2 i−1

j=1

Y2n,j

2

28ε−2 n=1

2−4n

2n

i=2

EXi2i−1

j=1

EXj2 (29)

212

15

ε−2 i=1

i−4EXi2i−1

j=1

EXj2

212

15

ε−2 i=1

i−2pEXipi−1

j=1

EXjp

214

15

ε−2 i=1

i−pE φpXi φp(i)+φpXii−1

j=1

jpE φpXj

φp(j)+φpXj<∞.

Similarly, in the case (b), we have

n=1

P

 2−2n

2n

i=2

Y2n,i i−1

j=1

Y2n,j

≥ε

212

15

ε−2 i=2

i−2pEXipi−1

j=1

EXjp

214

15

ε−2 i=2

i−pE φXi φ(i)+φXii−1

j=1

jpE φXj

φ(j)+φXj<∞.

(30)

Now using the Borel-Cantelli lemma we obtain 2−2n

2n

i=2

Y2n,i i−1

j=1

Y2n,j →0 a.s.,n → ∞. (31) Thus by (15) and (18) we see that

S2n

2n →0 a.s.,n → ∞, (32)

so we have

n−1

n i=1

Xi−EXi

→0 a.s.,n → ∞. (33)

But{Xn, n≥1}and{Xn, n≥1}are equivalent, so that n−1

n=1

Xi−EXi

→0 a.s.,n→ ∞ (34)

which completes to proof of Theorem 3.

(7)

Theorem 3 generalizes results of [2, 5, 10].

Before giving an example showing that the presented conditions under which WLLN is equivalent to the SLLN can be applied when some earlier known ones fail we quote the following results in this subject.

Theorem4[13]. Let{Xn, n≥1}be a sequence of independent-valued random variables such that

(a) Xj/j→0a.s.,j→ ∞,

(b) for somep∈[1,2]and somer∈(0,∞)

n=1

2 n+1 j=2n+1

EXjp/2(n+1)p

r

<∞. (35)

Then

Sn

n

P 0 if and only if Sn

n →0a.s.,n→ ∞. (36)

Theorem5[13]. Let{Xn, n≥1}be a sequence of independent-valued random variables such that

(a) |Xj| ≤Mj/LLjfor some constantM <∞, whereLLj=log(log(j∨ee)), and (b)

n=1{−ε/Λ(n)}<∞for allε >0whereΛ(n)=2n+1

j=2n+1EXj2/22(n+1). Then Sn

n

P 0 if and only if Sn

n →0a.s.,n→ ∞. (37)

Theorem6[15]. Let{Xn, n≥1}be a sequence of independentB-valued random variables, and let{an}and{bn}be constants that0< bn. Suppose that

(i)

i=2a2iXi

b4iφ(ai)

i−1

j=1

a2jXj

φ(aj) <∞ (ii) b12n

n

i=1a2iXi

φ(ai) 0, (iii)

i=1P(Xi> ai) <∞, (iv)

i=1a4iXi

b4iφ(ai) <∞.

ThenSn/bn P 0,if and only ifSn/bn→0a.s.,n→ ∞.

Example7. Let l2=

x=

xn, n≥1

R, x2= n=1

|xn|2<∞

(38) and leten denotes the element having 1 for itsnth coordinate and 0 in the other coordinates.

Assume thatn, n≥1}is a sequence of independent random variables such that P

ξ1=0

=1, P

ξj= ± j (LLj)2/(1+δ)

=(LLj)2+1 jlogj , P

ξj= ±j3

= 1

j1+δ, P ξj=0

=1− 2

j1+δ2(LLj)2+2 jlogj ,

(39)

(8)

j≥1,0< δ <1, and defineXnnen. We see that

n=1

2 n+1 j=2n+1

EXjp 2(n+1)p

r

=2 n=1

2 n+1 j=2n+1

jp/(LLj)2p/(1+δ)·

(LLj)2+1

/jlogj+j3p/j(1+δ) 2(n+1)p

r

2 n=1

2 n+1 j=2n+1

j3p−(1+δ) 2(n+1)p

r

2 n=1

2n·2n(3p−(1+δ))

2np2p r

= 2 2pr

n=1

2n(2p−δ)r= ∞.

(40)

Moreover, we note that the condition (a) of Theorem 5 (see [13]) is not satisfied.

Therefore neither Theorem 4 nor Theorem 5 can be applied in this case.

Now we state that the series (i) withφ(x)= |x|1+δ, 0< δ <1, bn=nandan= n/LLnin Theorem 6 (see [15]) can be written in the form

j=2

a2jEφXj j4φ(aj)

j−1

i=1

a2iEφXi φ(ai)

= j=3

j2 (LLj)2

j1+δ (LLj)2

·

(LLj)2+1 jlogj

+

j3(1+δ) j1+δ j4

j1+δ

(LLj)1+δ

×

j−1

i=2

i2 (LLi)2

i1+δ (LLi)2

·

(LLi)2+1 ilogi

+ i3(1+δ)

i1+δ i1+δ

(LLi)1+δ

j=3

j2 (LLj)2

·j2(1+δ) j4

j1+δ

(LLj)1+δ

j−1

i=1

i2 (LLi)2

i2(1+δ) i1+δ

(LLi)1+δ

j=3

jδ−1 (LLj)1+δ

j−1

i=1

i3+δ (LLi)1+δ

j=3

jδ−1 (LLj)1−δ

j3+δ (LLj)1+δ =

j=3

j2+2δ (LLj)2−2δ= ∞.

(41)

Thus we cannot also use Theorem 6.

But we can show that the assumptions of Theorem 3 are fulfiled as (A)

j=2j−2E φXj

φ(j)+φXjj−1

i=1i2E φXi

φ(i)+φXi

j=2j−2 1

jlogj + j(1+δ)1

j−1 i=1i2

× 1

ilogi+i(1+δ)1

<∞, (B) n−2n

i=1i2E φXi

φ(i)+φ

Xi≤n−2n

i=1i2 1

ilogi+i(1+δ)1

=o(1), (C)

n=1P

XnLLnn

=

n=1 1 n1+δ <∞, (D)

n=1φ(an)E φXn

φ(n)+φXn≤C

n=2

2

nlogn(LLn)1+δ+n3(1+δ)(LLn)1 1+δ

<∞.

(9)

Now it is enough to see that (4) holds. Taking into account that

n=1P[XnXn] <∞, we need only to verify that

P

n i=1

Xi−EXi ≥nε

→0, n → ∞. (42)

Using Chebyshev’s inequality and the fact thatl2is a space of the type 2, we have

P

n i=1

Xi−EXi ≥nε

≤C(ε)n

i=1

EXi2

n2 =o(1), (43)

which completes the proof that Sn

n →0 a.s.,n → ∞ (44)

Corollary8. If(B)and(B1)are replaced by the condition

n−1n

i=1

iEφXi φ(i)

=o(1), (45)

and in the case (b) additionallyEXk=0, k1, then Sn

n

P 0 a.s.,n → ∞if and only if Sn

n →0a.s.,n → ∞. (46) Proof. It is enough to show that the condition

n−1n

i=1

iEφXi φ(i)

=o(1) (47)

implies

n−1

n i=1

EXiIXi< i

→0, n → ∞. (48)

Indeed in the case (a) we have n−1

n i=1

EXiIXi< i =n−1

n i=1

iEXiIXi< i i

≤n−1 n i=1

iE

φXi φ(i)

=o(1),

(49)

while in the case (b), n−1

n i=1

EXiIXi< i =n−1

n i=1

iEXiIXi≥i i

≤n−1 n i=1

iE

φXi φ(i)

=o(1).

(50)

(10)

Corollary9. Let {Xn, n≥1} be a sequence of independent-valued random elements. If

j=2

j−2E Xj2 j2+Xj2

j−1

i=1

i2E Xi2 i2+Xi2<∞, n−2

n i=1

i2E Xi2

i2+Xi2=o(1),

n=1

PXn≥an

<∞

(51)

for some sequence{an, n≥1}of positive numbers with

n=1

a2nE Xn2

n4+Xn4<∞, (52)

then

n−1 n k=1

Xk−EXk P

0, n → ∞ (53) if and only if

n−1 n k=1

Xk−EXk

→0 a.s.,n → ∞. (54)

To prove the above-given assertion it is enough to use in the case (b) of the Theorem 3 the functionφ(x)=x2.

Corollary10. Let{Xn, n≥1}be a sequence of independent random elements in a Banach space ofα,0< α≤1 [12]. Suppose that in the case (a) the conditions (A), (B), (C) and (D) are satisfied withp=1+α, or in the case (b) the conditions(A1),(B1),(C), and(D1)are satisfied withp=1+α. Then

n−1 n k=1

Xk−EXk

→0 a.s.,n → ∞. (55)

Proof. It is enough to show that (4) holds. Indeed in the case (a), we get P

n k=1

Xk−EXk > nε

≤ε−2n−2E

n k=1

Xk−EXk

2

−2n−2 n k=1

EXk2

−2n−2 n k=1

kpE φpXk

φp(k)+φpXk=o(1),

(56)

and in the case (b), we have P

n k=1

Xk−EXk > nε

−2n−pn

k=1

kpE Xkp kp

−2n−p n k=1

kpE φXk

φ(k)+φXk=o(1).

(57)

(11)

But{Xn, n≥1}and{Xn, n≥1}are equivalent, therefore we have (4) which com- pletes the proof of Corollary 10.

Now we give a generalization of Theorem 3 replacing the condition (A) or(A1)by less restrictive ones.

We need the following lemma (see [6, page 329]).

Lemma11. Ifxj,1≤j≤n, are real numbers,Sn=n

j=1xjand

Qk,n=

1≤i1<i2<···<ik≤n

xi1xi2· ··· ·xik, 1≤k≤n, (58)

then for2≤k≤n, Qk,n=

n j=k

xjQk−1,j−1 and Snk=k!·Qk,n+ck, (59)

whereckis a generic designation for a finite linear combination (coefficients indepen- dent ofn) of termsm

j=1n

i=1xihj

of orderk, that is, m

j=1

hj=k, 1≤hj≤k,1≤m≤k. (60)

Using this lemma we can prove the following result.

Theorem12. Let{Xn, n≥1}be a sequence of independent-valued random ele- ments. Suppose that in the case (a) for somep, 1< p≤2,

(A)

jk=kjk−p(k−1)E φpX

jk

φp(jk)+φpX

jkjk−1

jk−1=k−1jpk−1 · E φpX

jk−1

φp(jk−1)+φpX

jk−1···

j2−1

j1=1j1pE φpXj

1

φp(j1)+φpXj

1<∞fork≥2

(B) and (C)–(D) are satisfied, or the case (b) for somep,1< p≤2, (A1)

jk=kjk−p(k−1)E φX

jk

φ(jk)+φX

jkjk−1

jk−1=k−1jk−1p · E φX

jk−1

φ(jk−1)+φX

jk−1···

j2−1

j1=1j1pE φXj

1

φ(j1)+φXj

1<∞, (B1), and (C)–(D1) are satisfied.

Then (4) holds if and only if (5) does.

Proof. Using Lemma 11 we get 2n−kS2n−ES2nk=

2−n

2n

i=1

Y2n,i

k

=

k−2

h=1

ch

2−n

2n

i=1

Y2n,i

h

Ak−h,2n+ckAk,2n+k!

2n−k Qk,2n,

(61)

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Weighted sums of independent and identically distributed random variables, weak law of large numbers, convergence in probability, random indices, strong law of large numbers,