Elsevier

Statistics & Probability Letters

Volume 69, Issue 3, 15 September 2004, Pages 261-269
Statistics & Probability Letters

Almost sure limit theorems for U-statistics

https://doi.org/10.1016/j.spl.2004.06.019Get rights and content

Abstract

We relax the moment conditions from a result in almost sure limit theory for U-statistics due to Berkes and Csaki [(Stochastic Process. Appl. 94 (2001) 105)]. We extend this result to the case of convergence to stable laws and also prove a functional version.

Introduction

U-statistics generalize the concept of the sample mean of independent identically distributed (i.i.d.) random variables. The statistical interest in U-statistics stems from the fact that they form a class of unbiased estimators of a certain parameter with minimal variances. We begin by introducing some notation and recalling the concept of U-statistics.

Let X1,X2,… be i.i.d random variables with common distribution function F(x). Let m⩾1 and let h:RmR be a measurable function symmetric in its arguments. The U-statistic with kernel h is defined byUn(h)=nm−11⩽i1<i2<⋯<im⩽nh(Xi1,…,Xim),n⩾m.The kernel h is called degenerate with respect to F(x) if for all 1⩽jm,Rh(x1,…,xm)dF(xj)≡0,where−∞<x1,…,xj−1,xj+1,…,xm<∞.Letθ=Eh(X1,…,Xm)and for i=0,…,m leth̄i(x1,…,xi)=Eh(x1,…,xi,Xi+1,…,Xm),hi(x1,…,xi)=k=0i(−1)i−k(j1,…,jk)⊂{1,…,i}h̄k(xj1,…,xjk),ζi=Var(hi(X1,…,Xi)).Note that h̄0 and h̄m(x1,…,xm)=h(x1,…,xm). Furthermore, the hi are degenerate for i=1,…,m (see Denker, 1985). If ζ1>0 the U-statistic Un(h) is called non-degenerate and degenerate otherwise. The smallest integer c for which ζc>0 is called the critical parameter of the U-statistic Un(h). Without loss of generality we will assume θ=0 throughout the rest of this article.

The theory of U-statistics started to develop intensively after Hoeffding's (1948) fundamental article. He showed asymptotic normality of non-degenerate U-statistics under the assumptionEh2(X1,…,Xm)<∞,using the following representation of U-statistics:Un(h)=mUn(h1)+k=2mmkUn(hk),where mUn(h1) is a sum of i.i.d. random variables and Un(h2),…,Un(hm) are U-statistics with degenerate kernels.

In the degenerate case nc/2Un(h) weakly converges to a multiple Wiener integral whenever h is square integrable (see e.g. Denker, 1985). Here c is the critical parameter of Un(h).

In the late 1980s, Brosamler (1988) and Schatte (1988) independently proved a new type of limit theorem. This type of statement extends the classical central limit theorem in the i.i.d. case to a pathwise version and is therefore called an almost sure central limit theorem (ASCLT). In the 1990s, many studies were done to prove almost sure limit theorems (ASLT) in different situations, for example in the case of independent but not necessarily identically distributed random variables (see Berkes and Dehling, 1993). Excellent surveys on this topic may be found in Atlagh and Weber (2000) as well as in Berkes (1998). Recently Berkes and Csaki (2001) obtained a general result in almost sure limit theory. They used it to prove almost sure versions of several classical limit theorems. In particular they stated the following theorem for U-statistics.

Theorem 1.1

Let c be the critical parameter of the U-statistic Un(h). Under assumption (1),limn→∞1lognk=1n1k1{kc/2Uk(h)<x}=G(x)a.s.foranyx∈CG,where G is the limit distribution of nc/2Un(h) and CG denotes the set of continuity points of G.

In the present note we relax the moment condition in Theorem 1.1 and extend the statement in two directions. First we will obtain an ASLT with stable limiting distribution for a non-degenerate U-statistic. Furthermore we extend Theorem 1.1 to a functional version.

Section snippets

Preliminaries

Let (Yn)n⩾1 be a sequence of random elements taking values in a Polish space (S,d) and let G be a probability measure on the Borel σ-field in S. We say that (Yn)n⩾1 satisfies the ASLT with limiting distribution G if with probability 1,(logn)−1k=1nδYk/k⇒G,n→∞.Here δYk is the Dirac measure at Yk and “⇒” denotes weak convergence of measures. Throughout this note the following lemma will be of fundamental interest.

Lemma 2.1

Let (Yn)n⩾1 be a sequence of S-valued random elements which satisfies the ASLT with

Relaxing the moment assumption

In this section, we will relax the moment assumption of Theorem 1.1. For the weak convergence of nc/2Un(h) (where c denotes the critical parameter of Un(h)) Koroljuk and Borovskich (1994) weakened assumption (1) toE|hk(X1,…,Xk)|2k/(2k−c)<∞,k=c,…,m.We are going to prove the validity of Theorem 1.1 under these assumptions:

Theorem 3.1

Let c be the critical parameter of the U-statistic Un(h). If (4) is satisfied then the statement of Theorem 1.1 is true.

Proof

First of all note that, if c is the critical parameter of

Convergence to stable distributions

As we shall see in this section, under some mild moment conditions weak convergence of a sequence of non-degenerate U-statistics to a stable limit distribution implies the validity of the corresponding ASLT. Let Gα denote a stable law with characteristic exponent α.

Theorem 4.1

Let for some α∈(1,2],n1−1/αmL(n)Un(h)−An⇒Gα,where L(n) is a slowly varying function for which liminfn→∞L(n)>0. IfE|hk(X1,…,Xk)|αk/(α(k−1)+1)<∞,k=2,…,m,thenlimn→∞1lognk=1n1k1{(k1−1/α)/Uk(h)/(mL(k))−Ak<x}=Gα(x)a.s.

Remarks

(1) Assumption (6)

The non-degenerate case

In the non-degenerate case the functional version of Theorem 1.1 can be deduced directly from Theorem 2 of Lacey and Philipp (1990), which deals with sums of i.i.d. random variables. Throughout this section we assume that (1) holds. Let D[0,1] denote the space of cadlag functions on [0,1] and let W denote the Wiener measure on D[0,1] (see Billingsley, 1999). We introduce the following D[0,1]-valued random functionsYn(t)=(m1)−1⌊nt⌋U⌊nt⌋(h):t∈[m/n,1],0:t∈[0,mn[,where ⌊·⌋ denotes the integer

Acknowledgements

We are grateful to H. Dehling for drawing our attention to a helpful publication by E. Giné and J. Zinn.

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Acknowledges the financial support of the graduate school Gruppen und Geometrie.

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Acknowledges the financial support of the graduate school Strömungsinstabilitäten und Turbulenz.

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