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Vol. 22, No. 1 (1999) 171–177 S 0161-17129922171-0

© Electronic Publishing House

MARCINKIEWICZ-TYPE STRONG LAW OF LARGE NUMBERS FOR DOUBLE ARRAYS OF PAIRWISE INDEPENDENT

RANDOM VARIABLES

DUG HUN HONG and SEOK YOON HWANG (Received 31 May 1996)

Abstract.Let Xij

be a double sequence of pairwise independent random variables.

If P

|Xmn| ≥t

≤P

|X| ≥t

for all nonnegative real numbers tandE|X|p

log+|X|3

<∞, for 1< p <2, then we prove that

m

i=1n j=1

Xij−EXij

(mn)1/p →0 a.s. asm∨n→ ∞. (0.1)

Under the weak condition ofE|X|plog+|X|<∞, it converges to 0 inL1. And the results can be generalized to anr-dimensional array of random variables under the conditions E|X|p

log+|X|r+1

<∞,E|X|p

log+|X|r−1

<∞, respectively, thus, extending Choi and Sung’s result [1] of the one-dimensional case.

Keywords and phrases. Strong law of large numbers, pairwise independent.

1991 Mathematics Subject Classification. 60F15.

1. Introduction. Etemadi [3] extended the classical law of large numbers for i.i.d.

random variables to the case where the random variables are pairwise i.i.d., i.e., if {Xn} is a sequence of pairwise i.i.d. random variables withE|X1|<∞, then

n

i=1

Xi−EXi

n →0 a.s. (1.1)

In 1985, Choi and Sung [1] have shown that if {Xn}are pairwise independent and are dominated in distribution by a random variable Xwith E|X|p

log+|X|2

<∞,1<

p <2, then ni=1n(X1/pi−EXi) →0 a.s. In addition, ifE|X|p<∞, then it converges to 0 in L1.

For a double sequence Xij

of pairwise i.i.d. random variables, also Etemadi [3]

proved that ifE|X11|log+|X11|<∞, then m

i=1n

j=1

Xij−EXij

mn →0 a.s. asm∨n → ∞. (1.2)

Now, we are interested in the extension of Choi and Sung’s result of the one- dimensional case to a multi-dimensional array of pairwise independent random vari- ables, which is established in the next section.

2. Main results. Let Xij

be a double sequence of random variables and letXij= XijI

|Xij| ≤(ij)1/p

, Xij=XijI

|Xij|> (ij)1/p

for 1< p <2. Throughout this paper,

(2)

c denotes an unimportant positive constant which is allowed to change and dkthe number of all divisors of integerk.

To prove the main theorem, we need the following lemmas.

Lemma2.1. Let Xij

be a double sequence of pairwise independent random vari- ables. If P

|Xmn| ≥t

≤P

|X| ≥t

for all nonnegative real numberst, then (a)

i=1

j=1

EXij2

(ij)2/p ≤cE|X|plog+|X|, (b)

i=1

j=1

EXij

(ij)1/p ≤cE|X|plog+|X| for1< p <2.

(2.1)

Proof. The estimation of E|Xij|2is given by

EXij2 (ij)2/p

0 P Xij2≥t dt

(ij)2/p

0 P |X|2≥t dt

= (ij)2/p

0

P t≤ |X|2< (ij)2/p

+P (ij)2/p≤ |X|2 dt

= (ij)1/p

0 x2dF(x)+(ij)2/pP (ij)2/p≤ |X|2 ,

(2.2)

where F(x)is the distribution ofX. If we use the fact that

k=i+1dk/k2/p=O logi/

(i+1)2/p−1

, we obtain

i=1

j=1

1 (ij)2/p

(ij)1/p

0 x2dF(x)≤c k=1

dk

k2/p k1/p

0 x2dF(x)

≤c i=0

k=i+1

dk

k2/p

(i+1)1/p

i1/p x2dF(x)

≤c i=0

logi (i+1)2/p−1

(i+1)1/p

i1/p x2dF(x)

≤cE|X|plog+|X|<∞.

(2.3)

And

i=1

j=1

P

(ij)2/p≤ |X|2

= k=1

dkP

k≤ |X|p

= k=1

k

j=1

dj

P

k≤ |X|p< k+1

=c k=1

klogkP

k≤ |X|p< k+1

≤cE|X|plog+|X|<∞,

(2.4)

(3)

where we use the fact thatn

k=1dk=O(nlogn). It follows that

i=1

j=1

EXij2

(ij)2/p <∞, which proves (a). (2.5) By the fact that n

k=1dk/k1/p =O

n1−(1/p)logn

, we can obtain (b) by the same method.

The following lemma is a two parameter analog of [5, Lem. 3.6.1a].

Lemma2.2. Let Xij

be a double sequence of pairwise independent random vari- ables with EXij=0, and letSmn=m

i=1n

j=1Xij. Then

E

max

1≤i≤m 1≤j≤n

Sij



2

≤c(logm)2(logn)2m

k=1

n l=1

EXkl2. (2.6) Proof. For m=1 and n=1, the inequality is trivial. If m >1, let sbe an integer such that 2s−1< m≤2s. And if n >1, let tbe an integer such that 2t−1< n≤2t. We can assume thatm, n >1. We assign Xijto the point (i,j)of integer in (0,2s]×(0,2t] (if m < i2s or n < j2t, setXij=0). Divide the interval(0,2s]into (0,2s−1]and (2s−1,2s], each of these two intervals into two halves, and so on. Then the elements of theith partition are of length 2s−i, i=0,...,s. Also, divide the interval(0,2t]in the same way. Then we obtain the(i,j)th partition Pij of(0,2s]×(0,2t]by theith partition of (0,2s] and the jth partition of (0,2t]. Every rectangle (0,i]×(0,j] is the sum of at most (s+1)(t+1)disjoint subrectangles each of which belongs to a different partition. We can write Sij =s

k=0

t

l=0Ykl;ij, where Ykl;ij is the sum of all r.v.’s belonging to the rectangle (a,b]×(c,d], b−a=2kand d−c=2l, which may or may not be a summand of (0,i]×(0,j]so that some Ykl;ij may vanish. Let Tij= 2i

k=1

2j

l=1|Ykl|2, where Yklis the sum of all r.v.’s which belong to the(k,l)-element of Pij. If we put T=s

i=0t

j=0Tij, by the elementary Schwarz inequality, we obtain Sij2≤(s+1)(t+1)

s k=0

t l=0

Ykl;ij2≤(s+1)(t+1)T . (2.7) SinceETijm

k=1n

l=1EXkl2, ET≤(s+1)(t+1)m

k=1n

l=1EXkl2. It follows that E

max

1≤i≤m 1≤j≤n

Sij2

≤(s+1)2(t+1)2 m k=1

n l=1

EXkl2

≤c(logm)2(logn)2m

k=1

n l=1

EXkl2.

(2.8)

Theorem2.3. Let Xij

be a double sequence of pairwise independent random vari- ables. If P

|Xmn| ≥t

≤P

|X| ≥t

for all nonnegative real numbers tandE|X|p log+

|X|3<∞, for 1< p <2, then

m∨nlim→∞

m

i=1n

j=1

Xij−EXij

(mn)1/p =0 a.s. (2.9)

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Proof. We denote bySmn=m

i=1n

j=1Xij, Smn =m

i=1n

j=1Xij. Then we obtain the inequalities

i=1

j=1

P

Xij=Xij

= k=1

dkP

|X11|> k1/p

k=1

dkP

|X|> k1/p

=

i=1

i

k=1

dk

(i+1)1/p

i1/p dF(x)

≤c i=1

ilogi

(i+1)1/p

i1/p dF(x)

≤cE|X|plog+|X|<∞,

(2.10)

Hence, by the Borel-Cantelli lemma, m

i=1

n

j=1

Xij−Xij

(mn)1/p →0 a.s. (2.11)

Now, we use Chebyshev’s inequality and Lemma 2.1 to obtain

k=1

l=1

P

S2k2l−ES2k2l

2k2l1/p > "

≤c k=1

l=1

VarS2k2l

2k2l2/p

=c k=1

l=1

1 2k2l2/p

2k

i=1 2l

j=1

VarXij

≤c i=1

j=1

EXij2 (ij)2/p

≤cE|X|plog+|X|p<∞,

(2.12)

which follows easily by summation by parts. It follows that S2k2l−ES2k2l

2k2l1/p →0 a.s. (2.13)

And let

Tkl= max

2k≤m<2k+1 2l≤n<2l+1

S2k2l

2k2l1/p Smn (mn)1/p

S2k2l

2k2l1/p+ max

2k≤m<2k+1 2l≤n<2l+1

Smn (mn)1/p,

(2.14)

whereSmn =Smn −ESmn .

By using Lemma 2.2, we obtain, for any" >0,

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k=0

l=0

P



 max

2k≤m≤2k+1 2l≤n≤2l+1

Smn (mn)1/p ≥"

2



≤c

k=0

l=0

1

2k2l2/pE



 max

2k≤m≤2k+1 2l≤n≤2l+1

Smn



2

≤c k=0

l=0

(k+1)2(l+1)2 2k+12l+12/p

2k+1

i=1 2l+1

j=1

EXij2

≤c i=1

j=1

(log2ij)2

(ij)2/p EXij2,

(2.15)

where the last inequality follows easily be summation by parts. But

i=1

j=1

(log2ij)2

(ij)2/p EXij2 k=1

dk(log2k)2 k2/p

k1/p

0 x2dF(x)

i=0

k=i+1

dk(log2k)2 k2/p

(i+1)1/p

i1/p x2dF(x)

≤c i=0

i1−(2/p)(logi)3

(i+1)1/p

i1/p x2dF(x)

≤cE|X|p

log+|X|p3

<∞,

(2.16)

where we use

k=1dk(log2k)2

k2/p =O i(logi)(2/p)−13

which follows by summation by parts.

Hence, (2.13), (2.15), and (2.16) give us Smn −ESmn

(mn)1/p →0 a.s. (2.17)

Combining (2.11) and (2.17), we get Smn−ESmn

(mn)1/p →0 a.s. (2.18)

Since

Smn−ESmn

(mn)1/p =Smn−ESmn (mn)1/p

m

i=1n

j=1EXij

(mn)1/p , (2.19)

it remains to prove that the second term of the right-hand side converges to 0 a.s. By Lemma 2.1(b), we obtain

k=1

l=1

2k

i=1

2l

j=1EXij 2k2l1/p ≤c

i,j=1

EXij (ij)1/p

≤cE|X|plog+|x|<∞,

(2.20)

from which, it follows that

k∨llim→∞

2k

i=12l

j=1EXij

2k2l1/p =0. (2.21)

(6)

But since

Tkl = max

2k≤m≤2k+1 2l≤n≤2l+1

m

i=1

n

j=1EXij (mn)1/p

2k i=1

2l

j=1EXij 2k2l1/p

c

2k+12l+11/p 2k+1

i=1 2l+1

j=1

EXij,

(2.22)

Tkl converges to 0 which implies that, by (2.21), m

i=1

n

j=1EXij

(mn)1/p →0. (2.23)

This completes the proof.

Corollary2.4. Let Xij

be a double sequence of pairwise i.i.d. random variables with E|X11|p

log+|X11|3

<∞, for1< p <2. Then

m∨nlim→∞

m

i=1n

j=1

Xij−EXij

(mn)1/p =0 a.s. (2.24)

Remark. The generalization tor-dimensional arrays of random variables can be obtained easily under the conditionE|X|p

log+|X|r+1<∞.

Theorem2.5. Let Xij

be a double sequence of pairwise independent random vari- ables. If P

|Xij| ≥t

≤P

|X| ≥t

for all nonnegative real numbers tand E|X|plog+

|X|<∞,1< p <2, then m

i=1n

j=1

Xij−EXij

(mn)1/p →0 inL1asm∨n → ∞. (2.25) Proof. Since

Xij

are pairwise independent,

Xij −EXij

are orthogonal which implies that

E

m

i=1n

j=1

Xij−EXij (mn)1/p

2

m

i=1n

j=1EXij2

(mn)2/p . (2.26)

Since

E

m

i=1n

j=1

Xij−EXij (mn)1/p

≤E

m

i=1n

j=1

Xij −EXij (mn)1/p

+2

m

i=1

n

j=1EXij (mn)1/p ,

(2.27)

it suffices to show that m

i=1n

j=1E|Xij|2

/(mn)2/p converges to 0 asm∨n →0.

But this can be shown by a method similar to that used in the proof of (2.23) in Theorem 2.3.

Corollary2.6. Let Xij

be a double sequence of pairwise i.i.d. random variable withE|X11|plog+|X11|<∞, for1< p <2. Then

m

i=1n

j=1

Xij−EXij

(mn)1/p →0 inL1asm∨n → ∞. (2.28)

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Remark. The generalization tor-dimensional arrays of random variables can be obtained under the conditionE|X|p

log+|X|r+1<∞.

Acknowledgement. This research was supported by the Catholic University of Taegu-Hyosung.

References

[1] B. D. Choi and S. H. Sung,On convergence of(Sn−ESn)/n1/r, 1< r <2, for pairwise independent random variables, Bull. Korean Math. Soc.22 (1985), no. 2, 79–82.

MR 87f:60044. Zbl 585.60043.

[2] K. L. Chung,A course in probability theory, second ed., Probability and Mathematical Sta- tistics, vol. 21, Academic Press, New York, 1974. MR 49 11579. Zbl 345.60003.

[3] N. Etemadi,An elementary proof of the strong law of large numbers, Z. Wahrsch. Verw.

Gebiete55(1981), no. 1, 119–122. MR 82b:60027. Zbl 448.60024.

[4] G. H. Hardy and E. M. Wright,An introduction to the theory of numbers, fourth ed., Claren- don Press, Oxford, 1960. Zbl 086.25803.

[5] M. Loeve,Probability theory. I, fourth ed., Graduate Texts in Mathematics, vol. 45, Springer- Verlag, New York, 1977. MR 58 31324a. Zbl 359.60001.

[6] R. T. Smythe,Strong laws of large numbers forr-dimensional arrays of random variables, Ann. Probability1(1973), no. 1, 164–170. MR 49 11602. Zbl 258.60026.

[7] W. F. Stout,Almost sure convergence, Probability and Mathematical Statistics, vol. 24, Aca- demic Press, New York, 1974. MR 56 13334. Zbl 321.60022.

Hong: School of Mechanical and Automotive Engineering, Catholic University of Taegu-Hyosung, Kyungbuk712-702, South Korea

Hwang: Department of Mathematics, Taegu University, Kyungbuk713-714, South Ko- rea

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Mathematical Problems in Engineering

Special Issue on

Modeling Experimental Nonlinear Dynamics and Chaotic Scenarios

Call for Papers

Thinking about nonlinearity in engineering areas, up to the 70s, was focused on intentionally built nonlinear parts in order to improve the operational characteristics of a device or system. Keying, saturation, hysteretic phenomena, and dead zones were added to existing devices increasing their behavior diversity and precision. In this context, an intrinsic nonlinearity was treated just as a linear approximation, around equilibrium points.

Inspired on the rediscovering of the richness of nonlinear and chaotic phenomena, engineers started using analytical tools from “Qualitative Theory of Di

erential Equations,”

allowing more precise analysis and synthesis, in order to produce new vital products and services. Bifurcation theory, dynamical systems and chaos started to be part of the mandatory set of tools for design engineers.

This proposed special edition of the Mathematical Prob-

lems in Engineering aims to provide a picture of the impor-

tance of the bifurcation theory, relating it with nonlinear and chaotic dynamics for natural and engineered systems.

Ideas of how this dynamics can be captured through precisely tailored real and numerical experiments and understanding by the combination of specific tools that associate dynamical system theory and geometric tools in a very clever, sophis- ticated, and at the same time simple and unique analytical environment are the subject of this issue, allowing new methods to design high-precision devices and equipment.

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Manuscript Due February 1, 2009 First Round of Reviews May 1, 2009 Publication Date August 1, 2009

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