Hindawi Publishing Corporation Journal of Applied Mathematics Volume 2014, Article ID 412758, 5 pages http://dx.doi.org/10.1155/2014/412758 Research Article A Strong Law of Large Numbers for Weighted Sums of i.i.d. Random Variables under Capacities Defei Zhang and Ping He School of Mathematics, Honghe University, Mengzi 661199, China Correspondence should be addressed to Ping He; [email protected] Received 16 February 2014; Accepted 3 June 2014; Published 16 June 2014 Academic Editor: Abdel-Maksoud A. Soliman Copyright © 2014 D. Zhang and P. He. 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. With the notion of independent identically distributed (i.i.d.) random variables under sublinear expectations initiated by Peng, a strong law of large numbers for weighted sums of i.i.d. random variables under capacities induced by sublinear expectations is obtained. 1. Introduction The strong law of large numbers plays important role in the development of probability theory and mathematical statistics; many studies about the extension of it have been completed by many authors. For example, Chow and Lai [1], Stout [2], Choi and Sung [3], Cuzick [4], Rosalsky and Sreehari [5], Wu [6], Bai and Cheng [7], Bai et al. [8], and so forth investigated the almost sure limiting behavior of weighted sums of i.i.d. random variables. In fact, the additivity of probability and expectations is not reasonable in many areas of applications because many uncertain phenomena cannot be well modeled using additive probabilities or linear expectations (see, e.g., Chen and Epstein [9], Huber and Strassen [10], and Wakker [11]). In the case of nonadditive probabilities, Marinacci [12] proved several limit laws for nonadditive probabilities and Maccheroni and Marinacci [13] obtained a strong law of large numbers for totally monotone capacities. Recently, motivated by the risk measures, superhedge pricing, and modelling uncertainty in finance, Peng [14] introduced the notion of sublinear expectation space, which is a generalization of probability space. Together with the notion of sublinear expectation, Peng also introduced the notions about i.i.d., πΊ-normal distribution, and πΊ-Brownian motion. Under this framework, the weak law of large numbers and the central limit theorems under sublinear expectations were obtained in the studies by Peng in [15, 16]. Soon thereafter, Denis et al. [17] introduced the function spaces and capacity related to a sublinear expectation. Chen et al. [18] proved a strong law of large numbers for nonadditive probabilities. A natural question is the following: can we investigate strong laws of large numbers for weighted sums of random variables under capacities? Indeed, the goal of this paper is to discuss the strong laws of large numbers for weighted sums of i.i.d. random variables under capacities. Under some assumptions, we obtain a strong law of large numbers for weighted sums of i.i.d. random variables under capacities. The paper is organized as follows: in Section 2, we give some definitions and lemmas that are useful in this paper. In Section 3, we give our main results including the proofs. 2. Preliminaries In this section, we present some preliminaries in the theory of sublinear expectations and capacities. More details of this section can be found in the studies by Chen et al. [18] and Peng [19]. Let (Ξ©, F) be a measurable space, and let H be the set of random variables on (Ξ©, F). Μ is a functional E Μ : Definition 1. A sublinear expectation E H β π satisfying the following: Μ Μ (i) monotonicity: E[π] β₯ E[π] if π β₯ π; Μ (ii) constant preserving: E[πΆ] = πΆ for πΆ β π ; 2 Journal of Applied Mathematics Μ + π] β€ E[π] Μ Μ (iii) subadditivity: E[π + E[π]; Μ Μ (iv) positive homogeneity: E[ππ] = πE[π] for π β₯ 0. Artzner et al. [20] showed that a sublinear expectation can be expressed as a supremum of linear expectations. That is, if Μ is a sublinear expectation on H, then there exists a set (say E P) of probability measures such that Μ [π] = sup πΈπ [π] , E Μ [βπ] = inf πΈπ [π] , βE πβP πβP βπ β H. (1) For this P, following Huber and Strassen [10], we define a pair (πΆ, πΆ) of capacities denoted by πΆ (π΄) := sup π(π΄) , πΆ (π΄) := inf π(π΄) , πβP πβP βπ΄ β F. (2) πΆ (π β π·, π β πΊ) = πΆ (π β π·) πΆ (π β πΊ) holds for both capacities πΆ and πΆ. Borel-Cantelli lemma is still true for capacities πΆ and πΆ under some assumptions. Lemma 6 (see Chen et al. [18]). Let {π΄ π , π β₯ 1} be a sequence of events in F. β β (1) If ββ π=1 πΆ(π΄ π ) < β, then πΆ(βπ=1 βπ=π π΄ π ) = 0. (3) where π΄ is the complement set of π΄. It is easy to check that πΆ and πΆ are two continuous capacities in the sense of the following definition. Definition 2. A set function πΆ: F β [0, 1] is called a continuous capacity if it satisfies (1) πΆ(π) = 0, πΆ(Ξ©) = 1; π=1 π=1 (7) β β If ββ π=1 πΆ(π΄ π ) = β, then πΆ(βπ=1 βπ=π π΄ π ) = 1. 3. Main Results Theorem 7. Let {ππ , π β₯ 1} be a sequence of i.i.d. random Μ 1 ], π = βE[βπ Μ variables in H satisfying π = E[π 1 ] and for any β, π > 0 (3) πΆ(π΄ π ) β πΆ(π΄), if π΄ π β π΄; (4) πΆ(π΄ π ) β πΆ(π΄), if π΄ π β π΄, where π΄ π , π΄ β F. π Μ [π(β|ππ | ) ] < β. E Definition 3 (see Peng [19]). Identical Distribution. Let π1 and π2 be two π-dimensional random vectors in H. They are called identically distributed, π denoted by π1 = π2 , if, for each measurable function π on π π such that π(π1 ), π(π2 ) β H, one has (5) Remark 4. A sequence of random variables {ππ , π β₯ 1} is said to be i.i.d., if ππ = π1 and ππ+1 is independent of π := (π1 , . . . , ππ ) for each π β₯ 1. The following lemma shows the relation between Pengβs independence and pairwise independence in the study by Marinacci in [12]. (8) Let {πππ , 1 β€ π β€ π, π β₯ 1} be an array of constants satisfying π΄ πΌ = lim supπ΄ πΌ,π < β, πββ π΄πΌπΌ,π = (4) Independence. A random vector π := (π1 , . . . , ππ ), ππ β H, is said to be independent of another random vector π := Μ if, for each measurable (π1 , . . . , ππ ), ππ β H, under E function π on π π × π π with π(π, π) β H and π(π₯, π) β H for each π₯ β π π , one has π β In this section, we give our main results including the proofs. (2) πΆ(π΄) β€ πΆ(π΅), whenever π΄ β π΅ and π΄, π΅ β F; Μ [π (π, π)] = E Μ [E[π Μ (π₯, π)] ] . E π₯=π β πΆ (βπ΄ππ ) = βπΆ (π΄ππ ) . π Μ [π (π1 )] = E Μ [π (π2 )] . E (6) (2) Suppose that {π΄ π , π β₯ 1} are pairwise independent with respect to πΆ; that is, Obviously, πΆ (π΄) + πΆ (π΄π ) = 1, Lemma 5 (see Chen et al. [18]). Suppose that π, π β H are Μ is a sublinear expectation and (πΆ, πΆ) two random variables. E Μ If random variable π is is the pair of capacities induced by E. Μ then π is also pairwise independent independent of π under E, of π under capacities πΆ and πΆ; that is, for all subsets π· and πΊ β π , σ΅¨ σ΅¨πΌ βππ=1 σ΅¨σ΅¨σ΅¨πππ σ΅¨σ΅¨σ΅¨ , π (9) (1 < πΌ β€ 2) . Then, for 0 < π β€ 1, if π (1 β lim sup πββ βππ=1 πππ ) β₯ 0, ππ (10) we have πΆ (π β€ lim inf πββ βππ=1 πππ ππ ππ βπ π π β€ lim sup π=1 ππ π β€ π) = 1, ππ πββ where ππ = π1/πΌ log1/π π. (11) Journal of Applied Mathematics 3 Moreover, for π > 1, if π(1βlim supπ β β (βππ=1 πππ /ππ )) β₯ 0, we have βππ=1 πππ ππ πΆ (π β€ lim inf πββ ππ π πΆ (lim supβπππ πππ > π) = 0 βπ > 0. π β β π=1 βπ π π β€ lim sup π=1 ππ π β€ π) = 1, ππ πββ (12) (1+(πΌβ1)(πβ1))/(1+πΌ(πβ1)) 1/πΌ Using Lemma 6, we have where ππ = π (log π) . In order to prove Theorem 7, we need the following lemma. Lemma 8. Let {ππ , π β₯ 1} be a sequence of i.i.d. random variables satisfying (8), and let {πππ , 1 β€ π β€ π, π β₯ 1} be an array of constants. Truncate |ππ β π| at Ξ π and denote πππ := (ππ β π)πΌ{|ππ βπ|β€Ξ π } . Suppose that the following conditions hold: (1) |πππ πππ | β€ πΆ|ππ |π½ / log π π.π . πΆ, for some 0 < π½ β€ π and some constant πΆ > 0; 2 2 βππ=1 πππ β€ π’π |ππ |πΏ / log π π.π . πΆ, for some πΏ > 0 (2) πππ and some sequence {π’π } of constants such that π’π β 0. The proof is complete. Proof of Theorem 7. The proof of (11) is similar to that of σΈ := (ππ β (12); we only prove (12). We denote πππ σΈ σΈ σΈ σΈ σΈ π)πΌ{|ππ βπ|β€(log π)πΏ1 } , πππ := (ππ β π)πΌ{|ππ βπ|β€(log π)1/π } , and πππ := (ππ β π)πΌ{(log π)πΏ1 β€|ππ βπ|β€(log π)1/π } for 1 β€ π β€ π and π β₯ 1, σΈ where πΏ1 = 1/(1 + πΌ(π β 1)). Denote πππ := πππ πΌ{|πππ |β€π1/πΌ (log π)πΏ2 } σΈ σΈ σΈ and πππ := πππ β πππ for 1 β€ π β€ π and π β₯ 1, where πΏ2 = (π β 1)/(1 + πΌ(π β 1)). Then, σΈ π σΈ βππ=1 πππ (ππ β π) βπ=1 πππ πππ βπ πσΈ σΈ πσΈ = + π=1 ππ ππ ππ ππ ππ + Then, π β β π=1 (13) Proof. From the inequality ππ₯ β€ 1 + π₯ + (1/2)π₯2 π|π₯| for all π₯ β π , we have Μ [π2 ππ‘|πππ πππ | ] Μ [ππ‘πππ πππ ] β€ 1 + 1 π‘2 π2 E E ππ 2 ππ (14) for any π‘ > 0. Let π > 0 be given. We set π‘ = 2 log π/π and obtain by (1) and (2) in Lemma 8 and (8) that σ΅¨σ΅¨ β1 σΈ σΈ σ΅¨σ΅¨ σ΅¨σ΅¨ππ πππ πππ σ΅¨σ΅¨ β€ σ΅¨ σ΅¨ π σΈ 2 σΈ 2 πππ β€ βππβ2 πππ π=1 β€ 2 π½ 2π’π log π πππ Μ [σ΅¨σ΅¨σ΅¨ππ σ΅¨σ΅¨σ΅¨πΏ π(2/π)πΆ|ππ | ] E π σ΅¨ σ΅¨ 2 2 π βπ=1 πππ 2 π½ 2πΆ π’ log π πππ Μ [ππΆ(π)|ππ | ] E β€ 1 + 1 π2 π 2 π βπ=1 πππ σ΅¨ σ΅¨πΌ π(2βπΌ)/πΌ βππ=1 σ΅¨σ΅¨σ΅¨πππ σ΅¨σ΅¨σ΅¨ (2βπΌ)πΏ2 ππ2 (log π) (2+πΌ(πβ1))/(1+πΌ(πβ1)) (log π) (19) ππ2 π΅π β€ ] σ΅¨ σ΅¨πΌ × βσ΅¨σ΅¨σ΅¨πππ σ΅¨σ΅¨σ΅¨ = π΄πΌπΌ,π = πβ3/2 . a.s. πΆ. Namely, πΆ (lim supπ΅π β€ π΄πΌπΌ,π ) = 1. (16) (21) π=1 πββ 2 log π πππ 1 π exp { } β 2 π2 π=1 2 βππ=1 πππ (20) (1+(πΌβ1)(πβ1))/(1+πΌ(πβ1)) (log) 1 π σ΅¨σ΅¨ σΈ σΈ σ΅¨σ΅¨ (log π) β σ΅¨σ΅¨π σ΅¨σ΅¨ β€ ππ π=1 σ΅¨ ππ σ΅¨ ππ π(πΌβ1)/πΌ π π=1 β€ a.s. πΆ. For π΅π , we observe that for all large π. For the large π, it follows by the Markov inequality and (15) that Μ [π πΆ (βπππ πππ > π) β€ πβπ‘π E σΈ 2 πππ π΄πΌπΌ,π πΏ π‘ βππ=1 πππ πππ a.s. πΆ, π πΆ (lim supπ΄ π > ) = 0 βπ > 0. 2 πββ (15) 2 log π πππ } π 2 2 βπ=1 πππ π σ΅¨ σ΅¨ σ΅¨σ΅¨ σ΅¨σ΅¨ σ΅¨σ΅¨σ΅¨ππ σ΅¨σ΅¨σ΅¨ π = σ΅¨ σ΅¨ π σ΅¨ σ΅¨ πΏ log π ππ (log π) 2 π1/πΌ Hence, by Lemma 8, we have 2 log π πππ β€1+ 2 2 βππ=1 πππ β€ exp { (18) For π΄ π , we will apply Lemma 8 to the random variable σΈ σΈ πππ and weight ππβ1 πππ . Note that 2 Μ [ππ‘πππ πππ ] β€ 1 + 2log π π2 E Μ 2 π‘|πππ πππ | ] E ππ [πππ π π2 β€1+ σΈ σΈ σΈ βππ=1 πππ πππ βπ π πσΈ σΈ + π=1 ππ ππ ππ ππ := π΄ π + π΅π + πΆπ + π·π . π πΆ (lim supβπππ πππ > π) = 0 βπ > 0. (17) (22) By replacing ππ by πππ (π > 0), we have lim supπ΅π β€ πββ π΄πΌπΌ,π π a.s. πΆ. (23) 4 Journal of Applied Mathematics Letting π β β, we have which implies πΆ (lim supπ΅π β€ 0) = 1. (24) πββ σ΅¨σ΅¨ π πσΈ σΈ σΈ σ΅¨σ΅¨ π΄ σ΅¨σ΅¨ ππ ππ σ΅¨σ΅¨ πΌ,π σ΅¨σ΅¨ σ΅¨σ΅¨π σ΅¨σ΅¨ σ΅¨ σ΅¨σ΅¨ ππ σ΅¨σ΅¨σ΅¨ β€ log π σ΅¨σ΅¨ππ σ΅¨σ΅¨ σ΅¨ σ΅¨ β€ βππ=1 πππ ππ > π) = 0. ππ (31) πΆ (lim sup βππ=1 πππ ππ β€ π) = 1. ππ (32) πββ For πΆπ , note that σΈ σΈ σΈ 2 π 2 πππ βπ=1 πππ 2 ππ πΆ (lim sup π΄2πΌ,π 2 log π Also, a.s. πΆ, σ΅¨σ΅¨ σ΅¨σ΅¨2π σ΅¨σ΅¨ππ σ΅¨σ΅¨ (25) a.s. πΆ. πββ Similarly, considering the sequence {βππ , π β₯ 1}, from (29), we have Then, by Lemma 8, we have π πΆ (lim supπΆπ > ) = 0 βπ > 0. 2 πββ (26) For π·π , assumption (8) implies βππ=1 πΆ(|ππ | > log1/π ) < σΈ σΈ | is bounded a.s. πΆ. It β. Hence, by Lemma 6, βππ=1 |πππ follows that σ΅¨ σΈ σΈ σ΅¨σ΅¨ σ΅¨ σ΅¨ σ΅¨σ΅¨ βππ=1 σ΅¨σ΅¨σ΅¨πππ σ΅¨σ΅¨σ΅¨ βππ=1 σ΅¨σ΅¨σ΅¨σ΅¨πππ σ΅¨ π·π β€ ππ β€ π΄ πΌ,π (1+(πΌβ1)(πβ1))/(1+πΌ(πβ1)) (log π) (27) π σ΅¨ σΈ σΈ σ΅¨σ΅¨ σ΅¨σ΅¨ σ³¨β 0 a.s. πΆ × β σ΅¨σ΅¨σ΅¨σ΅¨πππ σ΅¨ πΆ (lim sup πββ βππ=1 πππ (βππ ) Μ [βπ1 ]) = 1. β€E ππ Μ Note that π = βE[βπ 1 ]. So πΆ (lim sup πββ βππ=1 πππ ππ β₯ π) = 1. ππ (34) Therefore, the proof of Theorem 7 is complete. The following theorem shows that if the norming constant ππ is stronger than that of Theorem 7, then condition (8) in Theorem 7 can be replaced by a weaker condition. Theorem 9. Let {ππ , π β₯ 1} be a sequence of i.i.d. random Μ 1 ], π = βE[βπ Μ variables in H satisfying π = E[π 1 ] and for some β, π > 0 π=1 as π β β. Thus, π πΆ (lim supπ·π β€ 0) = 1. πββ (28) πββ βππ=1 πππ ππ β₯ π + π) ππ β€ πΆ (lim sup πββ πΆ (π β€ lim sup βππ=1 πππ (ππ β π) ππ β₯ π (1 β lim sup πββ βππ=1 πππ ) + π) ππ πββ (29) πββ πββ βππ=1 πππ ) + π) , ππ πββ βππ=1 πππ ππ β₯ π + π) = 0 βπ > 0, ππ βπ π π β€ lim sup π=1 ππ π β€ π) = 1, ππ πββ πΆ (π β€ lim sup and the condition π(1 β lim supπ β β βππ=1 πππ /ππ ) β₯ 0: from (20), (24), (26), and (28), we conclude that πΆ (lim sup (35) βππ=1 πππ ππ ππ where ππ = π1/πΌ (log π)1/π+π½ . Moreover, for π > 1 and π½ lim supπ β β (βππ=1 πππ /ππ )) β₯ 0, we have = πΆ (lim sup (π΄ π + π΅π + πΆπ + π·π ) β₯ π (1 β lim sup Μ [π(β|ππ | ) ] < β. E Let {πππ , 1 β€ π β€ π, π β₯ 1} be an array of constants satisfying (9) in Theorem 7. Then, for 0 < π β€ 1 and π½ > 0, if π(1 β lim supπ β β (βππ=1 πππ /ππ )) β₯ 0, we have On the other hand, βπ > 0; and we note that πΆ (lim sup (33) (30) πββ > 0, if π(1 β βππ=1 πππ ππ ππ βπ π π β€ lim sup π=1 ππ π β€ π) = 1, ππ πββ where ππ = π1/πΌ (log π)(1+(πΌβ1)(πβ1))/(1+πΌ(πβ1))+π½ . (36) (37) Journal of Applied Mathematics 5 Proof. We can prove that Lemma 8 is also true except that (8) and (1) of Lemma 8 are replaced by (35) and the following condition. |πππ πππ | β€ Vπ |ππ |π½ / log π a.s. πΆ, for some 0 < π½ β€ π and some sequence {Vπ } of constants such that Vπ β 0. σΈ = ππ πΌ{|ππ |β€(ββ1 log π)1/π } and For the case 0 < π β€ 1, we let πππ σΈ σΈ σΈ πππ = ππ β πππ for 1 β€ π β€ π and π β₯ 1. For the case π > 1, we σΈ σΈ σΈ let πππ = ππ πΌ{|ππ |β€(log π)1/(1+πΌ(πβ1)) } , πππ = ππ πΌ{|ππ |>ββ1 log1/π π} , and σΈ σΈ σΈ πππ = ππ πΌ{(log π)1/(1+πΌ(πβ1)) <|ππ |β€(ββ1 log π)1/π } . The rest of the proof is similar to that of Theorem 7 and is omitted. Remark 10. If π = π = 0 in Theorem 9, then, for 0 < π β€ 1 and π½ > 0, we have βππ=1 πππ ππ σ³¨β 0 a.s., ππ (38) where ππ = π1/πΌ (log π)1/π+π½ . Moreover, if π > 1, we have βππ=1 πππ ππ σ³¨β 0 a.s., ππ (39) where ππ = π1/πΌ (log π)(1+(πΌβ1)(πβ1))/(1+πΌ(πβ1))+π½ . Since if πΌ > 1 and π β₯ 1, then π(πΌ β 1)/πΌ(1 + π) > 0 and (1 + (πΌ β 1)(π β 1))/(1 + πΌ(π β 1)) < 1/π + π(πΌ β 1)/πΌ(1 + π), we also have βππ=1 πππ ππ σ³¨β 0 a.s., ππ (40) where ππ = π1/πΌ (log π)1/π+π(πΌβ1)/πΌ(1+π) . The result is similar to Theorem 2.2 of Bai and Cheng [7]. Remark 11. If π = π = 0 in Theorem 7, we can get the classical strong law of large numbers for weighted sums of i.i.d. random variables as follows: βππ=1 πππ ππ = 0) = 1. πββ ππ π ( lim (41) Conflict of Interests The authors declare that there is no conflict of interests regarding the publication of this paper. Acknowledgments The authors thank Professor Zengjing Chen for his helpful discussion and suggestions and the reviewers for their valuable comments and suggestions to improve the presentation of this paper. This work is partially supported by the National Science Foundation of China (11301160), the Scientific Research Foundation of Yunnan Province (2013FZ116), the Scientific Research Foundation of Yunnan Province Education Committee (2011C120), the Reserve Talents Foundation of Honghe University (2014HB0204), and the Curricula Construction Foundations of Honghe University (ZYDT1308, ZDKC1111). References [1] Y. S. Chow and T. L. 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