Abstract
In this paper, we derive the weak and strong results of Marcinkiewicz–Zygmund laws of large numbers under sublinear expectation. The results are extensions of the Kolmogorov laws of large numbers under sublinear expectation and the classical Marcinkiewicz–Zygmund laws of large numbers.
1. Introduction
The theory of sublinear expectation was initiated by Peng [1, 2] to describe the probability uncertainties in statistics, economics, finance, and other fields which are difficult to be handled by the classical probability theory. The classical laws of large numbers (LLNs for short) which reveal the almost sure laws of stabilized partial sum are of great significance in the probability theory. Recently, the LLNs under sublinear expectation got a lot of development, see for example, Marinacci [3]; Maccheroni and Marinacci [4]; Chen et al. [5]; Chen [6]; Zhang [7]; Hu [8]; Chen et al. [9]; and Hu [10].
Peng [11]; Chen et al. [9]; and Hu [12] gave three forms of weak LLNs under sublinear expectation under the first moment condition. That is, for any ,for any ,and for any where denotes the pair of the sublinear expectation and the conjugate expectation and represent the induced capacities, and .
Chen et al. [5] obtained the Kolmogorov strong LLNs under sublinear expectation under the condition of finite th moments for sublinear expectation:
Zhang [7] got the above strong LLNs under the condition of finite first moment for Choquet expectation. Hu [8] improved the above results under a general moment condition for sublinear expectation which is the weakest one for sublinear expectation.
The classical Marcinkiewicz–Zygmund strong LLNs generalized the Kolmogorov strong LLNs by extending the convergence rate of partial sum and give the relation between moment conditions and convergence rate. The norming constants become instead of n and the moment conditions depend on p accordingly. In sublinear situation, Feng and Lan [13] obtained the Marcinkiewicz–Zygmund strong LLNs for arrays of row wise independent random variables. Zhang and Lin [14]; Xu and Zhang [15] got the Marcinkiewicz–Zygmund strong LLNs under the condition of finite pth moments for Choquet expectation by different methods. We know that Choquet expectation is larger than sublinear expectation. The purpose of this paper is to generalize the weak and strong LLNs to the Marcinkiewicz–Zygmund LLNs under some moment conditions for sublinear expectation. We discuss the weak results under the condition of p-order uniform integrability for sublinear expectation and study the strong results under the condition a bit stronger than finite pth moments for sublinear expectation.
The plan of this paper is as follows. In Section 2, we introduce the basic concepts and lemmas under sublinear expectation. In Section 3, we prove some forms of Marcinkiewicz–Zygmund weak LLNs under sublinear expectation and discuss the equivalence relation among them. In Section 4, the Marcinkiewicz–Zygmund strong LLNs under sublinear expectation is given.
2. Preliminaries
Let be a measurable space and be a linear space of real functions defined on such that if then for each where denotes the linear space of local Lipschitz continuous functions φ satisfyingfor some , depending on φ. contains all where . We also denote as the linear space of bounded Lipschitz continuous functions φ satisfyingfor some .
Definition 1. A function : is said to be a sublinear expectation if it satisfies for ,(a)Monotonicity: implies (b)Constant preserving: , (c)Positive homogeneity: , (d)Subadditivity: whenever is not of the form or The triple is called the sublinear expectation space.
Remark 1. By Definition 1, we can obtain two properties of sublinear expectation :(1)(2)
Remark 2. Let be a family of probability measures defined on . For any random variable , the upper expectation defined by is a sublinear expectation. So, the results in this paper can also be applied to upper expectation.
The conjugate expectation of is defined byObviously, for all , .
Definition 2 (see [16]). A set function is called a capacity if it satisfies(a)(b)In this paper, we consider the capacities induced by sublinear expectation and the conjugate expectation: , , .
The continuity from above and continuity from below of sublinear expectation and capacity can also be defined similar to the classical probability theory (see [7]).
Definition 3. (independence). is said to be independent of , if for each test function whenever the sublinear expectations on both sides are finite.
is said to be a sequence of independent random variables, if is independent of for each .
Remark 3. Peng [2] also gave the definition of identical distribution under the sublinear expectation space. The results in this paper do not need the random variables to be identically distributed.
To prove our main results, we need the following lemmas. The proofs of Lemma 1, Lemma 2, and Lemma 3 can be found in [5] and [8].
Lemma 1 (Borel–Cantelli lemma). If sublinear expectation is continuous from below and , then
Lemma 2 (Chebyshev’s inequality). Let be a nondecreasing function on . Then, for any real x,
Lemma 3. If , then .
In the following sections, we consider the sequence of independent random variables defined on a sublinear expectation space with , for each . Denote , .
3. The Marcinkiewicz–Zygmund Weak LLNs
Theorem 1. (1)If for some , then for any ,and for any ,(2)If for some , then
Proof. (1)For the case , we only give the proof of (11). The proof of (12) is similar to Theorem 3.1 of Hu [10], so we omit it. For any fixed , define a nondecreasing function such that when , when , and when . It is obvious that and . It follows that Let . By the independence of , we have Therefore, For any , there exist two random variables satisfying Thus, by , for any , we have Let . It follows that Then, by the arbitrariness of δ, we obtain Considering , applying the above consequence, we have Equivalently, Noting that , we obtain (11).(2)For the case , applying the function in (1) (actually, we only need here), we haveAlso, by, we getFor any , there exists some random variables satisfyingSo, for any ,By the arbitrariness of δ, we obtainConsidering , we have
Theorem 2. For any , the following two statements are equivalent:(1)For any ,(2)For any ,
Proof. (1) ⟹ (2) : Let , then for any ,By the arbitrariness of ε and the continuity of φ, we obtain expression (30).
(2) ⟹ (1) : For any , define a function as follows:We can easily obtain that and . Then,Theorem 1 together with Theorem 2 gives birth to the following result.
Corollary 1. If , for some , , for each when . Then, for any ,
Remark 4. If sublinear expectation coincides with the classical expectation where P is classical probability, (11)–(13) and (34) all can be reduced to the classical forms.
4. The Marcinkiewicz–Zygmund Strong LLNs
To study the moment conditions for strong LLNs, we need the following concept of function class which was introduced by Petrov [17]. Let (or, respectively, ) denote the set of nonnegative functions defined on satisfying(1) is positive and nondecreasing on . The series converges (respectively, diverges).(2)For any fixed , there exists such that for any .
Functions and are examples of . The functions and belong to .
Before we give the main results, we need the following two lemmas which are used to cope with the truncated parts.
Lemma 4. Suppose that . Then, for any ,
Proof. Since , we have for each . The rest of the proof is similar to Lemma 2.5 of Hu [8].
Lemma 5. Suppose that for some , andThen, for any , we have
Proof. Since for all real x, and for ,we have for any ,Taking expectations, for ,Since , the function converges to as . Then, for any ,For , by noting thatwe haveFor , by noting thatwe haveWe set a such that , i.e., . So, for , we haveThen, there exists some such that for any ,By the independence of , we have
Theorem 3. Suppose that is continuous from below.(1)If for some and , then(2)If for some and , then
Proof. (1)For, define and . Then, . Let and denote . Then, Note that Therefore, We can easily obtain that are independent; , and . For any , we set . Then, by Chebyshev’s inequality, By Lemma 5 and , we have By Borel–Cantelli lemma, we have The continuity from below of can be deduced by the continuity from below of . So, we have Moreover, where By Lemma 4, we have By Kronecker lemma, we have On the other hand, by the continuity from below of , Then, by Lemma 3, we have which implies Taking on both sides of (54), and by (58), (62), and (65), we have Equivalently, Considering with , we have Equivalently, Noting that , we obtain (49).(2)For , let and denote . Then,We can easily obtain that are independent, , , and .
For any , we set . Then, by Chebyshev’s inequality and Lemma 5, we haveBy Borel–Cantelli lemma, we haveHence, by the continuity from below of , we haveLet for . Then,By Borel–Cantelli lemma, we haveThen, for any , there exists such that for any , . For these ω,Hence,which impliesFurthermore,which impliesTaking on both sides of (70) and by (73), (78), and (80), we haveEquivalently,Considering , we have
Remark 5. The two moment conditions for case and case in Theorem 3 are both stronger than but weaker than . Zhang and Lin [14] obtained that the pth moments for Choquet expectation is the necessary and sufficient conditions of the Marcinkiewicz–Zygmund strong LLNs. One can find a counterexample that the pth moments for sublinear expectation is finite but the pth moments for Choquet expectation is not finite (similar to Example 4.1 of Hu [12]. So the pth moments for sublinear expectation cannot maintain the Marcinkiewicz–Zygmund strong LLNs.
Remark 6. If sublinear expectation coincides with the classical expectation where P is classical probability, Theorem 3 can be reduced to the classical Marcinkiewicz–Zygmund strong LLNs:where if and if .
Data Availability
No data were used to support this study.
Conflicts of Interest
The authors declare no conflicts of interest.
Acknowledgments
This research was partially supported by the Natural Science Foundation of Shandong Province (no. ZR2019BA038).