Hindawi Publishing Corporation Discrete Dynamics in Nature and Society Volume 2010, Article ID 218380, 15 pages doi:10.1155/2010/218380 Research Article Convergence Properties for Asymptotically almost Negatively Associated Sequence Xuejun Wang, Shuhe Hu, and Wenzhi Yang School of Mathematical Science, Anhui University, Hefei 230039, China Correspondence should be addressed to Shuhe Hu, hushuhe@263.net Received 20 July 2010; Revised 9 October 2010; Accepted 2 November 2010 Academic Editor: Ibrahim Yalcinkaya Copyright q 2010 Xuejun Wang et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited. We get the strong law of large numbers, strong growth rate, and the integrability of supremum for the partial sums of asymptotically almost negatively associated sequence. In addition, the complete convergence for weighted sums of asymptotically almost negatively associated sequences is also studied. 1. Introduction Definition 1.1. A finite collection of random variables X1 , X2 , . . . , Xn is said to be negatively associated NA if, for every pair of disjoint subsets A1 , A2 of {1, 2, . . . , n}, Cov fXi : i ∈ A1 , g Xj : j ∈ A2 ≤ 0, 1.1 whenever f and g are coordinate-wise nondecreasing such that this covariance exists. An infinite sequence {Xn , n ≥ 1} is NA if every finite subcollection is NA. The concept of negative association was introduced by Joag-Dev and Proschan 1 and Block et al. 2. By inspecting the proof of maximal inequality for the NA random variables in Matuła 3, one also can allow negative correlations provided they are small. Primarily motivated by this, Chandra and Ghosal 4, 5 introduced the following dependence. Definition 1.2. A sequence {Xn , n ≥ 1} of random variables is called asymptotically almost negatively associated AANA if there exists a nonnegative sequence qn → 0 as n → ∞ such that 1/2 Cov fXn , gXn1 , Xn2 , . . . , Xnk ≤ qn Var fXn Var gXn1 , Xn2 , . . . , Xnk 1.2 2 Discrete Dynamics in Nature and Society for all n, k ≥ 1 and for all coordinate-wise nondecreasing continuous functions f and g whenever the variances exist. The family of AANA sequence contains NA in particular, independent sequences with qn 0, n ≥ 1 and some more sequences of random variables which are not much deviated from being negatively associated. An example of an AANA sequence which is not NA was constructed by Chandra and Ghosal 4. Since the concept of AANA sequence was introduced by Chandra and Ghosal 4, many applications have been found. For example, Chandra and Ghosal 4 derived the Kolmogorov-type inequality and the strong law of large numbers of MarcinkiewiczZygmund, Chandra and Ghosal 5 obtained the almost sure convergence of weighted averages, Ko et al. 6 studied the Hájek-Rényi-type inequality, and Wang et al. 7 established the law of the iterated logarithm for product sums. Recently, Yuan and An 8 established some Rosenthal-type inequalities for maximum partial sums of AANA sequence. As applications of these inequalities, they derived some results on Lp convergence, where 1 < p < 2, and complete convergence. In addition, they estimated the rate of convergence in Marcinkiewicz-Zygmund strong law for partial sums of identically distributed random variables. The main purpose of the paper is to study the strong law of large numbers, strong growth rate, and the integrability of supremum for AANA sequence. In addition, the complete convergence for weighted sums of AANA sequence is also studied. Throughout the paper, we let {Xn , n ≥ 1} be a sequence of AANA random variables . defined on a fixed probability space Ω, F, P . Denote Sn ni1 Xi . Let X a −aIX < −a XI|X| ≤ a aIX > a for some a > 0, and let IA be the indicator function . of the set A. For p > 1, let q p/p − 1 be the dual number of p. We assume that φx is a positive increasing function on 0, ∞ satisfying φx ↑ ∞ as x → ∞ and ψx is the inverse function of φx. Since φx ↑ ∞, it follows that ψx ↑ ∞. For easy notation, we let φ0 0 and ψ0 0. The an Obn denotes that there exists a positive constant C such that |an /bn | ≤ C. C denotes a positive constant which may be different in various places. The main results of this paper are dependent on the following lemmas. Lemma 1.3 cf. Yuan and An 8, Lemma 2.1. Let {Xn , n ≥ 1} be a sequence of AANA random variables with mixing coefficients {qn, n ≥ 1}, and let f1 , f2 , . . . be all nondecreasing (or nonincreasing) functions, then {fn Xn , n ≥ 1} is still a sequence of AANA random variables with mixing coefficients {qn, n ≥ 1}. Lemma 1.4. Let 1 < p ≤ 2, and let {Xn , n ≥ 1} be a sequence of AANA random variables with mixing coefficients {qn, n ≥ 1} and EXn 0 for each n ≥ 1. If ∞ 2 < ∞, then there exists a positive constant Cp depending only on p such n1 q n that n E max|Si |p ≤ Cp E|Xi |p 1≤i≤n for all n ≥ 1, where Cp 2p 22−p p 6pp i1 ∞ n1 p/q q2 n . 1.3 Discrete Dynamics in Nature and Society 3 Proof. We use the same notations as that in the study by Yuan and An 8. They proved that p p n n−1 p p 2−p 2/q Emax Si ≤ 2 p Xi p 6p q iXi p , 1≤i≤n i1 i1 p p n n−1 p p 2−p 2/q q iXi p , Emax−Si ≤ 2 p Xi p 6p 1≤i≤n i1 1.4 i1 p p max|Si |p ≤ 2p−1 max Si 2p−1 max−Si . 1≤i≤n 1≤i≤n 1≤i≤n By 1.4 and Hölder’s inequality, we have p p E max|Si |p ≤ 2p−1 Emax Si 2p−1 Emax−Si 1≤i≤n 1≤i≤n ≤2 p 2−p 2 ⎡ 1≤i≤n p n n p p 2/q p E|Xi | 6p q iXi p i1 i1 ⎤ p/q n n n p ≤ 2p ⎣22−p p E|Xi |p 6p q2 i E|Xi |p ⎦ i1 i1 1.5 i1 ⎡ p/q ⎤ ∞ n n p ⎦ E|Xi |p Cp E|Xi |p . ≤ 2p ⎣22−p p 6p q2 n n1 i1 i1 This completes the proof of the lemma. We point out that Lemma 1.4 has been studied by Yuan and An 8. But here we give the accurate coefficient Cp . And Lemma 1.4 generalizes and improves the result of Lemma 2.2 in the study by Ko et al. 6. Lemma 1.5 cf. Fazekas and Klesov 9, Theorem 2.1 and Hu et al. 10, Lemma 1.5. Let {Xn , n ≥ 1} be a sequence of random variables. Let b1 , b2 , . . . be a nondecreasing unbounded sequence of positive numbers, and let α1 , α2 , . . . be nonnegative numbers. Let r and C be fixed positive numbers. Assume that, for each n ≥ 1, n E max|Sl |r ≤ C αl , 1≤l≤n ∞ αl l1 1.6 l1 blr < ∞, 1.7 then lim Sn n → ∞ bn 0 a.s., 1.8 4 Discrete Dynamics in Nature and Society and with the growth rate βn Sn a.s., O bn bn 1.9 where βn max bk vkδ/r , ∀0 < δ < 1, 1≤k≤n vn ∞ αk br kn k , βn 0, n → ∞ bn lim r n Sl αl E max ≤ 4C r < ∞, b 1≤l≤n bl l1 l r ∞ Sl αl ≤ 4C E sup r < ∞. b b l l≥1 l1 l 1.10 If further one assumes that αn > 0 for infinitely many n, then r ∞ Sl αl < ∞. E sup ≤ 4C βr l≥1 βl l1 l 1.11 Lemma 1.6 cf. Fazekas and Klesov 9, Corollary 2.1 and Hu 11, Corollary 2.1.1. Let b1 , b2 , . . . be a nondecreasing unbounded sequence of positive numbers, and let α1 , α2 , . . . be nonnegative numbers. Denote Λk α1 α2 · · · αk for k ≥ 1. Let r be a fixed positive number satisfying 1.6. If ∞ Λl l1 1 1 − r blr bl1 < ∞, Λn is bounded, bnr 1.12 1.13 then 1.8–1.11 hold. Lemma 1.7 cf. Yuan and An 8, Theorem 2.1. Let {Xn , n ≥ 1} be a sequence of AANA random variables with EXi 0 for all i ≥ 1 and p ∈ 3 · 2k−1 , 4 · 2k−1 , where integer number k ≥ 1. If ∞ q/p n < ∞, then there exists a positive constant Dp depending only on p such that, for all n1 q n ≥ 1, E max|Si |p 1≤i≤n ⎧ n ⎨ p/2 ⎫ n ⎬ E|Xi |p EXi2 . ≤ Dp ⎩ i1 ⎭ i1 1.14 Discrete Dynamics in Nature and Society 5 Lemma 1.8. Assume that the inverse function ψx of φx satisfies ψn If Eφ|X| < ∞, then n 1 On. ψi i1 ∞ n1 1/ψnE|X|I|X| 1.15 > ψn < ∞. Proof. Since ψx is an increasing function of x, we have that ∞ ∞ ∞ 1 1 E|X|I |X| > ψn E|X|I ψi < |X| ≤ ψi 1 ψn ψn in n1 n1 ∞ i 1 E|X|I ψi < |X| ≤ ψi 1 ψn i1 n1 ≤ ∞ i 1 P ψi < |X| ≤ ψi 1 ψi 1 ψn i1 n1 ≤C 1.16 ∞ P ψi < |X| ≤ ψi 1 i i1 ≤ CE φ|X| < ∞. The proof is complete. 2. Strong Law of Large Numbers and Growth Rate for AANA Sequence Theorem 2.1. Let {Xn , n ≥ 1} be a sequence of mean zero AANA random variables with ∞ 2 n1 q n < ∞, and let {bn , n ≥ 1} be a nondecreasing unbounded sequence of positive numbers; 1 < p ≤ 2. Assume that ∞ E|Xn |p p n1 bn < ∞, 2.1 then lim Sn n → ∞ bn 0 a.s., 2.2 and with the growth rate βn Sn O a.s., bn bn 2.3 6 Discrete Dynamics in Nature and Society where βn max bk vkδ/2 , ∀0 < δ < 1, 1≤k≤n ∞ αk vn p kn bk , lim βn n → ∞ bn 0, αk Cp E|Xk |p , k ≥ 1, Cp is defined in Lemma 1.4, p n Sl αl E max ≤ 4 p < ∞, 1≤l≤n bl b l1 l p ∞ Sl αl ≤4 E sup p < ∞. b l l≥1 l1 bl 2.4 If further one assumes that αn > 0 for infinitely many n, then p ∞ Sl αl ≤4 E sup p < ∞. l≥1 βl l1 β 2.5 l Proof. By Lemma 1.4, we have n n E max |Sk |p ≤ Cp E|Xk |p αk . 1≤k≤n k1 2.6 k1 It follows from 2.1 that ∞ αn p n1 bn Cp ∞ E|Xn |p p n1 bn < ∞. 2.7 Thus, 2.2–2.5 follow from 2.6, 2.7, and Lemma 1.5 immediately. We complete the proof of the theorem. Theorem 2.2. Let {Xn , n ≥ 1} be a sequence of AANA random variables with 1 ≤ p < 2. Denote Qn max1≤k≤n EXk2 for n ≥ 1 and Q0 0. Assume that ∞ Qn < ∞, 2/p n1 n ∞ n1 q2 n < ∞, 2.8 then n 1 Xi − EXi 0 n → ∞ n1/p i1 lim a.s., 2.9 Discrete Dynamics in Nature and Society 7 and with the growth rate n βn 1 − EX O X i i n1/p i1 n1/p 2.10 a.s., where βn max k1/p vkδ/2 , 1≤k≤n ∀0 < δ < 1, vn ∞ αk , 2/p k kn βn 0, n → ∞ n1/p lim αk C2 kQk − k − 1Qk−1 , k ≥ 1, C2 is defined in Lemma 1.4, n S l 2 αl E max 1/p < ∞, ≤4 2/p 1≤l≤n l l1 l ∞ S l 2 αl ≤4 E sup 1/p < ∞. 2/p l l l≥1 l1 2.11 2.12 2.13 If further one assumes that αn > 0 for infinitely many n, then 2 ∞ Sl αl ≤4 < ∞. E sup 2 β l l≥1 l1 βl 2.14 ∞ S l r 4r αl ≤1 E sup 1/p < ∞. 2/p 2 − r l1 l l≥1 l 2.15 In addition, for any r ∈ 0, 2, Proof. Assume that EXn 0, bn n1/p , and Λn that n l1 αl , n ≥ 1. By Lemma 1.4, we can see 2 ⎞ k n n αk . E⎝ max Xi ⎠ ≤ C2 EXi2 ≤ C2 nQn 1≤k≤n i1 i1 k1 ⎛ 2.16 It is a simple fact that αk ≥ 0 for all k ≥ 1. It follows from 2.8 that ∞ l1 Λl 1 1 − 2 2 bl bl1 C2 ∞ l1 lQl 1 l2/p − 1 l 12/p ≤ ∞ 2C2 Ql < ∞. p l1 l2/p 2.17 8 Discrete Dynamics in Nature and Society That is to say that 1.12 holds. By Remark 2.1 in Fazekas and Klesov 9, 1.12 implies 1.13. By Lemma 1.6, we can obtain 2.9–2.14 immediately. By 2.13, it follows that ∞ ∞ S l r S l r Sl 1/r dt P sup 1/p > t dt ≤ 1 P sup 1/p > t E sup 1/p l l l 0 l≥1 1 l≥1 l≥1 ∞ ∞ S l 2 αl 4r ≤ 1 E sup 1/p t−2/r dt ≤ 1 < ∞. 2/p 2 − r l l 1 l≥1 l1 2.18 The proof is complete. Theorem 2.3. Let p ∈ 3 · 2k−1 , 4 · 2k−1 , where integer number k ≥ 1, and let {Xn , n ≥ 1} be q/p n < ∞. Let a sequence of AANA random variables with EXi 0 for all i ≥ 1 and ∞ n1 q {bn , n ≥ 1} be a nondecreasing unbounded sequence of positive numbers. Assume that ∞ p/2−1 n p bn n1 ∞ E|Xk | ∞ np/2−2 p k1 E|Xn |p < ∞, p bn nk1 2.19 < ∞, then 1.8–1.11 hold (for C 1), where ⎛ α1 2Dp E|X1 |p , ⎞ k−1 k p p αk 2Dp ⎝kp/2−1 EXj − k − 1p/2−1 EXj ⎠, j1 k ≥ 2, 2.20 j1 and Dp is defined in Lemma 1.7. Proof. Since p > 2, 0 < 2/p < 1. By Cr ’s inequality, n 2/p |Xi | p ≤ i1 n Xi2 , 2.21 i1 which implies that n i1 n E|Xi | ≤ E Xi2 p p/2 . 2.22 i1 By Jensen’s inequality, we have p/2 p/2 n n 2 2 EXi ≤E Xi . i1 i1 2.23 Discrete Dynamics in Nature and Society 9 By 2.22-2.23 and Cr ’s inequality, n E|Xi |p i1 n p/2 EXi2 p/2 n n 2 ≤ 2E Xi ≤ 2np/2−1 E|Xi |p . i1 i1 2.24 i1 It follows from Lemma 1.7 and 2.24 that n n αl . E max |Si |p ≤ 2Dp np/2−1 E|Xi |p 1≤i≤n i1 2.25 l1 It is a simple fact that ⎞ ⎛ k−1 p 0 ≤ αk ≤ C1 p ⎝kp/2−1 E|Xk |p kp/2−2 EXj ⎠, 2.26 j1 where C1 p is a positive number depending only on p and Dp . By 2.19, ∞ ∞ p/2−1 ∞ n np/2−2 p p E|Xk | < ∞. p ≤ C1 p p E|Xn | p n1 bn n1 bn k1 nk1 bn ∞ αn 2.27 The desired results follow from 2.25–2.27 and Lemma 1.5 immediately. 3. Complete Convergence for Weighted Sums of AANA Random Variables Theorem 3.1. Let {X, Xn , n ≥ 1} be a sequence of identically distributed AANA random variables 2 2 with ∞ n1 q n < ∞, EX 0, EX < ∞, and Eφ|X| < ∞. Assume that the inverse function ψx of φx satisfies 1.15. Let {ani , n ≥ 1, i ≥ 1} be a triangular array of positive constants such that i max1≤i≤n ani O1/ψn, ii ni1 a2ni Olog−1−α n for some α > 0. Then, for any ε > 0, ∞ n1 −1 n P j max ani Xi > ε < ∞. 1≤j≤n i1 3.1 10 Discrete Dynamics in Nature and Society Proof. For each n ≥ 1, denote n Xj −ψnI Xj < −ψn Xj I Xj ≤ ψn ψnI Xj > ψn , n j Tj n ani Xi n − Eani Xi ! 1 ≤ j ≤ n, 1 ≤ j ≤ n, , i1 A n " n Xi Xi ! i1 n " |Xi | ≤ ψn , i1 BA n # n Xi / Xi ! i1 j max ani Xi > ε . 1≤j≤n i1 n # |Xi | > ψn , i1 En 3.2 It is easy to check that j n ani Xi Tj i1 j j n Eani Xi ani Xi I |Xi | > ψn i1 j i1 ani ψn I Xj < −ψn − I Xj > ψn , i1 j n n maxT Eani Xi > ε En B 1≤j≤n j i1 En En A En B 3.3 j n n maxTj > ε − max Eani Xi B. 1≤j≤n 1≤j≤n i1 ⊂ Therefore, j n n maxTj > ε − max Eani Xi P B 1≤j≤n 1≤j≤n i1 P En ≤ P j n n n maxTj > ε − max Eani Xi P |Xi | > ψn . 1≤j≤n 1≤j≤n i1 i1 ≤P 3.4 Firstly, we will show that j n max Eani Xi −→ 0, 1≤j≤n i1 as n −→ ∞. 3.5 Discrete Dynamics in Nature and Society 11 It follows from Lemma 1.8 and Kronecker’s lemma that n 1 E|X|I |X| > ψi −→ 0, ψn i1 as n −→ ∞. 3.6 By EX 0, condition i, 3.6, and ψn ↑ ∞, we can see that j n n n Eani Xi I |Xi | ≤ ψn ani ψnEI |Xi | > ψn max Eani Xi ≤ i1 1≤j≤n i1 i1 ≤ n n ani E|Xi |I |Xi | > ψn ani E|Xi |I |Xi | > ψn i1 ≤ 3.7 i1 n C E|X|I |X| > ψi −→ 0, ψn i1 as n −→ ∞, which implies 3.5. By 3.4 and 3.5, we can see that, for sufficiently large n, j n n ε max ani Xi > ε ≤ P maxTj > P |Xi | > ψn . 1≤j≤n 1≤j≤n 2 i1 i1 P 3.8 To prove 3.1, it suffices to show that n ε n P maxTj > < ∞, 1≤j≤n 2 n1 ∞ −1 ∞ n n−1 P |Xi | > ψn < ∞. n1 3.9 i1 By Markov’s inequality, Lemma 1.4, Cr inequality, EX 2 < ∞, and condition ii, we have n ε n P maxTj > 1≤j≤n 2 n1 ∞ −1 ≤C ∞ ∞ n n 2 n 2 n−1 E maxTj ≤ C n−1 Eani Xi 1≤j≤n n1 ≤C ≤C ≤C ∞ n n1 i1 n−1 n1 i1 ∞ n a2ni EX 2 I |X| ≤ ψn C n−1 a2ni ψ 2 nEI |X| > ψn n1 i1 ∞ ∞ n n n−1 a2ni EX 2 I |X| ≤ ψn C n−1 a2ni EX 2 I |X| > ψn n1 i1 ∞ n ∞ n1 i1 n1 n−1 n1 a2ni ≤ C n−1 log−1−α n < ∞. i1 3.10 12 Discrete Dynamics in Nature and Society It follows from Eφ|X| < ∞ that ∞ ∞ ∞ n n−1 P |Xi | > ψn P |X| > ψn P φ|X| > n n1 i1 n1 3.11 n1 ≤ CE φ|X| < ∞. Theorem 3.2. Let {Xn , n ≥ 1} be a sequence of AANA random variables, and let {ani , n ≥ 1, i ≥ 1} be an array of positive numbers. Let {bn , n ≥ 1} be an increasing sequence of positive integers, and let {cn , n ≥ 1} be a sequence of positive numbers. If, for some p ∈ 3 · 2k−1 , 4 · 2k−1 , where integer number k ≥ 1, 0 < t < 2, and for any ε > 0, the following conditions are satisfied: bn ∞ ! cn P |ani Xi | ≥ εbn1/t < ∞, n1 ∞ bn −p/t c n bn n1 ∞ ∞ n1 ! |ani |p E|Xi |p I |ani Xi | < εbn1/t < ∞, 3.12 i1 −p/t c n bn n1 and i1 b ! p/2 n 2 2 1/t ani EXi I |ani Xi | < εbn < ∞, i1 qq/p n < ∞, then ⎧ ⎫ ∞ ⎨ ⎬ !% i $ 1/t 1/t ≥ εbn < ∞. anj Xj − anj EXj I anj Xj < εbn cn P max ⎩1≤i≤bn j1 ⎭ n1 3.13 Proof. Note that if the series ∞ holds. Therefore, we will n1 cn is convergent, then 3.13 consider only such sequences {cn , n ≥ 1} for which the series ∞ n1 cn is divergent. Let n Yi ! ! ! −εbn1/t I ani Xi < −εbn1/t ani Xi I |ani Xi | < εbn1/t εbn1/t I ani Xi > εbn1/t , Sni i n Yj , 3.14 n ≥ 1, i ≥ 1. j1 Note that ⎧ ⎨ ⎫ ⎬ !% i $ P max anj Xnj − anj EXj I anj Xj < εbn1/t ≥ εbn1/t ⎩1≤i≤bn j1 ⎭ ≤C bn ! −p/t P |ani Xi | ≥ εbn1/t 2p ε−p bn i1 E max |Sni − ESni | 1≤i≤bn 3.15 p . Discrete Dynamics in Nature and Society 13 n Using the Cr inequality and Jensen’s inequality, we can estimate E|Yi following way: n p − EYi | in the ! ! p/t n n p EYi − EYi ≤ C|ani |p E|Xi |p I |ani Xi | < εbn1/t Cbn P |ani Xi | ≥ εbn1/t . 3.16 By 3.15, 3.16, and Lemma 1.7, we can get ⎧ ⎨ ⎫ ⎬ !% i $ P max anj Xj − anj EXj I anj Xj < εbn1/t ≥ εbn1/t ⎩1≤i≤bn j1 ⎭ ≤C bn bn ! ! −p/t P |ani Xi | ≥ εbn1/t Cbn |ani |p E|Xi |p I |ani Xi | < εbn1/t i1 3.17 i1 −p/t Cbn b n p/2 a2ni EXi2 I |ani Xi | < εbn1/t ! . i1 Therefore, we can conclude that 3.13 holds by 3.12 and 3.17. Theorem 3.3. Let 1 ≤ r ≤ 2 and let {Xn , n ≥ 1} be a sequence of AANA random variables with EXn 0 and E|Xn |r < ∞ for n ≥ 1. Let {ani , n ≥ 1, i ≥ 1} be an array of real numbers satisfying the condition n ! |ani |r E|Xi |r O nδ as n −→ ∞ 3.18 i1 q/p and ∞ n < ∞ for some 0 < δ ≤ 2/p and p ∈ 3 · 2k−1 , 4 · 2k−1 , where integer number k ≥ 1. n1 q Then, for any ε > 0 and αr ≥ 1, ⎞ i nαr−2 P ⎝max anj Xj ≥ εnα ⎠ < ∞. 1≤i≤n n1 j1 ∞ ⎛ 3.19 14 Discrete Dynamics in Nature and Society Proof. Take cn nαr−2 , bn n, and 1/t α in Theorem 3.2. By 3.18, we have bn ∞ ∞ ∞ n ! |ani |r E|Xi |r cn P |ani Xi | ≥ εbn1/t ≤ C nαr−2 ≤ C n−2δ < ∞, αr n n1 i1 n1 i1 n1 ∞ ∞ ∞ n ! n−2 |ani |r E|Xi |r ≤ C n−2δ < ∞, |ani |p E|Xi |p I |ani Xi | < εbn1/t ≤ bn −p/t c n bn n1 i1 n1 i1 n1 p/2 b ∞ ∞ n ! p/2 n −p/t 2 r r 2 1/t αr−2−αrp/2 c n bn ani EXi I |ani Xi | < εbn ≤C n |ani | E|Xi | n1 i1 n1 ≤C ∞ i1 αr−2−αrp/2δp/2 n n1 ≤C ∞ nαr1−p/2−1 < ∞ n1 3.20 following from δp/2 ≤ 1. By the assumption EXn 0 for n ≥ 1 and 3.18, we get i 1 α anj EXj I anj Xj < εn max nα 1≤i≤n j1 ≤ n n 1 anj EXj I anj Xj < εnα 1 anj EXj I anj Xj ≥ εnα nα j1 nα j1 ≤ n 1 anj r EXj r ≤ Cnδ−αr −→ 0, nαr j1 3.21 as n −→ ∞ following from δ < 1 and αr ≥ 1. We get the desired result from Theorem 3.2 immediately. The proof is complete. 2 Theorem 3.4. Let {Xn , n ≥ 1} be a sequence of AANA random variables satisfying ∞ n1 q n < ∞, and let {ani , n ≥ 1, i ≥ 1} be an array of positive numbers. Let {bn , n ≥ 1} be an increasing sequence of positive integers, and let {cn , n ≥ 1} be a sequence of positive numbers. If, for some 1 < p ≤ 2, 0 < t < 2, and for any ε > 0, the following conditions are satisfied: bn ∞ ! cn P |ani Xi | ≥ εbn1/t < ∞, n1 ∞ i1 bn −p/t c n bn |ani |p E|Xi |p I n1 i1 ! 3.22 |ani Xi | < εbn1/t < ∞, then ⎧ ⎫ ∞ ⎨ ⎬ !% i $ anj Xj − anj EXj I anj Xj < εbn1/t ≥ εbn1/t < ∞. cn P max ⎩1≤i≤bn j1 ⎭ n1 Proof. 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