1. Introduction
The weak law of large numbers ensures that the sample mean converges in probability to the expected value, forming the foundation of consistent estimation. Under the independent and identically distributed (i.i.d. for short) setting, classical results are systematically presented in [
1], and may be outlined as follows.
Theorem 1. Let be a sequence of i.i.d. random variables. Then as , Let
and
be a slowly varying function. Ref. [
2] provided an extension of Theorem 1 to a more general case, as described below.
Theorem 2. Let be a sequence of i.i.d. random variables. Then as , The Gut’s law stated in Theorem 2 was generalized by [
3] to cover negatively associated (NA for short) random variables as well as the exponent regime
. Further extensions can be found in [
4,
5,
6,
7,
8,
9] for instance. Very recently, ref. [
10] made the first extension of Gut’s law to
-convergence (
) concerning maximum weighted sums of NA random variables, assuming that the weight sequence obeys
.
A further approach to extending the weak law of large numbers consists of deriving analogous results for
d-dimensional index arrays. Denote by
the set of
d-dimensional lattice points with positive integer coordinates, where
. Define a componentwise partial order “⪯” on
; i.e., for
and
,
(or
) implies that
for each
. Denote
. Consider a
d-dimensional random field
. Ref. [
11] studied an array of pairwise independent random variables in
d dimensions under stochastic domination by
X, and obtained that the condition
yields
Ref. [
12] established the
(
) convergence for multidimensional arrays of pairwise negatively quadrant dependent (NQD for short) random variables that are stochastically dominated in the Cesàro sense by a random variable
X. They also relaxed the moment condition to
as
.
In many applications, however, the observations are not identically distributed and are influenced by a non-uniform weight field . For example, consider a two-dimensional random field representing daily rainfall measurements at grid points . The weights can model directional or distance-based attenuation of sensor signals. The total impact on a distributed system is a weighted sum . Under this circumstance, traditional unweighted results fail to capture the influence of non-homogeneous weights. Moreover, Gut’s condition with would substantially weaken the tail requirements on the dominating variable X, making the law of large numbers applicable to a wider class of heavy-tailed distributions where (see Example 1, where the advantage of Gut’s condition is demonstrated).
The main contribution of this work is twofold: (i) extending the results of [
10] from NA random variables to multidimensional arrays of pairwise NQD random variables under Gut’s condition, and (ii) improving the
-convergence and weak law results of [
12] from partial sums to weighted sums.
To end this section, let us recall some concepts which are indispensable to illustrate our main results. Ref. [
13] proposed the following concept of stochastic domination in the Cesàro sense.
Definition 1. A d-dimensional random field is stochastically dominated in the Cesàro sense by X if, for some , the inequalityholds for every and . The Cesàro-type stochastic domination introduced above is strictly weaker than the standard stochastic domination, yet it is insufficient for deriving our main results. To address this issue, we propose a new notion of stochastic domination in the Cesàro sense relative to a given array.
Definition 2. Let . A random field is said to be stochastically dominated in the Cesàro sense by a random variable X with respect to the array if there exists a finite positive constant M such that for all and , Remark 1. Observe that when for every , Definition 2 reduces to the original Cesàro-type stochastic domination in Definition 1. Moreover, it is worth noting that the usual stochastic domination (i.e., for all and x) also implies the Cesàro-type stochastic domination in Definition 2 with respect to any weight array . Indeed, if holds for each , then summing over gives .
The notion of pairwise NQD random variables was introduced by [
14] as follows.
Definition 3. Two random variables X and Y are called NQD ifA sequence is said to be pairwise NQD if every pair of variables in the sequence satisfies this NQD property. It is worth noting that negatively orthant dependent, negatively superadditive dependent, NA, or pairwise independent sequences all belong to the class of pairwise NQD variables. Hence, this class is quite broad, and investigating its limit properties is of great significance. Extensive limit theorems have been established for pairwise NQD random variables, including the Kolmogorov strong law of large numbers for identically distributed sequences by [
15]; the Marcinkiewicz-type strong law under suitable conditions by [
16]; strong stability for Jamison-type weighted product sums by [
17]; maximal moment inequalities by [
18]; limit theorems by [
19]; the Hájek–Rényi-type inequality by [
20]; strong laws under normalizing sequences by [
21]; and complete moment convergence for weighted sums by [
22], among others. Ref. [
12] generalized the pairwise NQD concept to the multidimensional array setting.
Definition 4. A d-dimensional random field is termed pairwise NQD if for every pair of distinct indices and any real numbers ,
According to [
12], this dependence structure appears in many natural examples, including the cone measure and the volume measure on the ball of
.
We also recall the definition of a slowly varying function. A positive measurable function
on
is called slowly varying if, for any
,
Clearly, many functions are slowly varying, e.g.,
,
, and
with arbitrary
; here,
and
denotes the natural logarithm.
Finally, we establish the following notational conventions. C denotes a generic positive constant that may vary across occurrences. means ; indicates and . Moreover, , , with being the indicator of event A.
3. Some Important Lemmas
Prior to presenting the proofs of our main theorems, we need the following auxiliary results.
Lemma 1. If X and Y are NQD random variables, then for any nondecreasing (or nonincreasing) functions f and g, the transformed variables and remain NQD.
Lemma 2. Let be a pairwise NQD random field and a family of monotone functions (all nondecreasing or all nonincreasing). Then the transformed field is also pairwise NQD.
Proof. For any two distinct indices , the random variables and are pairwise NQD by definition. Therefore, it follows from Lemma 1 that and are also pairwise NQD. This verifies the lemma immediately. □
Ref. [
26] established the following von Bahr–Esseen-type inequality.
Lemma 3. Let be pairwise NQD random variables with zero means and finite p-th moments for some . Then there exists a constant depending only on p such that Lemma 4. Let be a d-dimensional pairwise NQD random field with and for some . Then for some constant (depending only on p), the following inequality holds for every : Proof. Write
and
. Define the finite set of indices
Noting that there exists a bijection
, we define for each
that
. Therefore, for every original index
, there is a unique
j such that
. Actually, the random variables are merely relabeled and thus the one-dimensional sequence
is still pairwise NQD by the definition of NQD random variables. Hence, applying Lemma 3 and observing that
is bijection, we can obtain
The proof is complete. □
Lemma 5. Suppose is a random field that is stochastically dominated in the Cesàro sense by X with respect to the constant array . Then for any positive constants a and b, Proof. It follows from Definition 2 and the fact
that
Moreover, by virtue of
and Definition 2 again, we have that
The proof is completed. □
The last lemma can be found in Lemma 1.2 of [
10] as follows.
Lemma 6. Let be slowly varying. Assume (after possibly replacing by with an appropriate C) that for some sufficiently large, the function is strictly increasing on and is strictly decreasing on . Then the following asymptotic equivalences hold.
(i) For and , we have .
(ii) For and , we have .
(iii) If , and , , then for all , 4. Proofs
Before presenting the detailed proofs, we briefly comment on the key technical novelties that allow us to go beyond the existing frameworks.
∗Multidimensional NQD inequality via bijection. In Lemma 4, we reduce the moment estimate for a d-dimensional array to the one-dimensional von Bahr–Esseen inequality by simply relabeling the index set through a bijection . This elementary trick makes the whole proof essentially as simple as the one-dimensional case, while still valid for all .
∗
Cesàro stochastic domination with weights. Lemma 5, built on Definition 2, provides the crucial bounds
and a similar bound for the truncated part. This allows us to replace the original weighted variables by those dominated by
X, while keeping the weight structure intact. Consequently, the dependence on the specific distributions of
is eliminated, and only the tail of
X matters.
With these points in mind, we now proceed to the rigorous proofs.
Proof of Theorem 3. Since
for each
, one can first prove
and
which together with the fact that
yields that
Since both
and
consist of non-negative coefficients, it is enough to establish the statement for non-negative coefficients
; the general case is then handled by applying the result to the positive and negative parts separately and taking the difference (the required conditions carry over because
, and the pairwise NQD property is preserved under the nondecreasing transformations
, see Lemma 2). Consequently, we can assume, with no loss of generality, that
holds for every
and
. For each
, denote
where
,
is a field of constants and
is a sequence of positive numbers diverging to infinity. It is sufficient to demonstrate that for every
,
and
It is straightforward to confirm (
1) via
that
For (
2), noting by Lemma 2 that
is still pairwise NQD, a combination of Markov inequality, Lemma 4,
and
gives
Finally, it follows from
again that
This establishes (
3), thereby concluding the proof. □
Proof of Corollary 1. To derive Corollary 1, it is enough to check that conditions
and
of Theorem 3 are satisfied with
. Actually, it follows from
and
as
that for all
, there is
such that
As
is arbitrary, this verifies condition
immediately. Similarly, for condition
, by virtue of Lemma 5 and the procedure above, we also have
Therefore, the proof of Corollary 1 is completed. □
Proof of Theorem 4. It may also be assumed without loss of generality that
for each
,
. For given
, we define
It follows from Lemma 2 that the zero-mean property and pairwise NQD dependence are preserved for both
and
over
,
. Using Hölder’s inequality
,
with
,
, and
, we have that for any
,
We first consider the case
. Choose
and
. On one hand, it follows from Lemma 4,
-inequality, Jensen’s inequality, Lemma 5, and (
4) that
The convergence to zero of the second term in the last line of (
5) follows from the hypothesis that
when
. Thus, in what follows, we will deal with the first term. Actually, it is evident that
It follows from Lemma 6 that
and for each fixed
,
Hence, we obtain by the Toeplitz lemma and the assumption
as
that
which together with (
6) derives that the first term in the last line of (
5) converges to zero.
On the other hand, applying Lemma 4, the
-inequality, Jensen’s inequality, Lemma 5, and (
4) once more yields
Thanks to (
6) and (
7), the first term in the last line of (
8) is seen to converge to zero. Therefore, the rest of the proof focuses on the second term. The convergence
as
implies that, for any
, we can choose
(depending only on
) so that
holds for each
. By the fact that
and Lemma 6, we have that for all
,
which, together with the arbitrariness of
, verifies that the second term of (
8) converges to zero.
Consequently, in view of the arguments above, we apply
-inequality and Jensen’s inequality to obtain
The argument for the case
is thereby completed.
For
, note that
It follows from (
5)–(
7) that as
,
and
Moreover, noting that
, by (
8), one can also verify that
□
Proof of Theorem 5. Let
. Note that
and
, so
and
. We begin with the decomposition
For
, we apply the inequality
for
to the inner sum, then use the fact that the maximum over
is bounded by the sum over the full index set
. This yields
which together with Jensen’s inequality yields
Applying inequality
to
gives
Both bounds now involve only sums over the full index set
, with the dependence on the partial index
completely removed. The rest of the argument coincides precisely with that of Theorem 4: apply Lemma 5 to replace
by
X, use the moment condition
to control the weight sums, and employ the slicing argument together with the Toeplitz lemma and the assumption
to show that both
and
converge to zero as
. □