A Koopman-von Neumann type theorem on the convergence of Cesàro means in Riesz spaces

By Jonathan Homann, Wen-Chi Kuo, and Bruce A. Watson

Abstract

We extend the Koopman-von Neumann convergence condition on the Cesàro mean to the context of a Dedekind complete Riesz space with weak order unit. As a consequence, a characterisation of conditional weak mixing is given in the Riesz space setting. The results are applied to convergence in .

1. Introduction

The Koopman-von Neumann Lemma, as referred to by Petersen Reference 14, Section 2.6 (see also Krengel Reference 7, Section 2.3, as well as Eisner, Farkas, Haase and Nagel Reference 3, Section 9.2), characterises the convergence to zero of the Cesàro mean of bounded, non-negative sequences of real numbers in terms of the existence of a convergent subsequence of the given sequence. Here, the subsequence is formed from the given sequence by the omission of a, so called, density zero set from , the index set of the given sequence.

In this paper, we consider the order convergence to zero of the Cesàro mean of an order bounded, non-negative sequence in a Dedekind complete Riesz space with weak order unit. This requires a more sophisticated density zero concept. In particular, we introduce a density zero sequence of band projections which forms the foundation for the Koopman-von Neumann condition in Riesz spaces. When the Riesz space is the real numbers the characterisation presented here gives the classical Koopman-von Neumann convergence condition.

As an application of the Koopman-von Neumann Lemma (Theorem 3.2), we give, in Section 4, a characterisation of conditional weak mixing in Riesz spaces. In Section 5, as an example, we apply Theorem 3.2 to characterise the order convergence of the Cesàro mean to zero of order bounded, non-negative sequences in . We also refer the reader to the recent work of Gao, Troitsky and Xanthos on the UO-convergence and its application to Cesàro means in Banach lattices Reference 5.

This work supplements the development of stochastic processes in Riesz spaces of Grobler Reference 6, Stoica Reference 15, Azouzi et al Reference 2, Kuo, Labuschagne and Watson Reference 9, and mixing processes in Riesz spaces as considered in Kuo, Rogans and Watson Reference 11, and Kuo, Vardy and Watson Reference 12.

2. Preliminaries

We refer the reader to Aliprantis and Border Reference 1, Fremlin Reference 4, Meyer-Nieberg Reference 13, and Zaanen Reference 18 and Reference 19, for background in Riesz spaces and -algebras.

We recall that, in a Riesz space, , a sequence in converges to zero, in order, if and only if the sequence converges, in order, to zero in . Further to this, in a Dedekind complete Riesz space, the absolute order convergence of a sum implies the order convergence of the sum, see below.

Lemma 2.1.

Let be a sequence in , a Dedekind complete Riesz space, then order convergence of implies the order convergence of .

Proof.

Suppose that , in order, as . Then is an upper bound for the increasing sequences , which, from the Dedekind completeness of , have order limits, say, . Thus, , in order, as .

From Reference 10, Lemma 2.1, we have the following theorem.

Theorem 2.2.

Let be a Dedekind complete Riesz space and a sequence in with , in order, as , then in order, as .

Corollary 2.3.

Let be a Dedekind complete Riesz space and a sequence in with order limit , then we have in order, as .

Proof.

Let for each , then is order convergent to , by assumption. Thus, by Theorem 2.2,

in order, as , and the result follows as is Archimedean.

3. The Koopman-von Neumann condition

In Reference 14, a subset of is said to be of density zero if as , where if and if . The Koopman-von Neumann Lemma Reference 14, Lemma 6.2 asserts that if a sequence of non-negative real numbers is bounded, then as if and only if there is , a subset of , of density zero, such that as , .

We recall that the subspace of consisting of the bounded elements of is an -algebra, see Reference 2Reference 16Reference 18. For all band projections and on , we set . Here, represents the -algebra multiplication on . The linear extension of this multiplication and use of order limits extends this multiplication to the -algebra multiplication on . Further, the weak order unit, , is the multiplicative unit of the -algebra.

In a Riesz space, , for , is called a component of if , see Reference 19, pg. 213. Furthermore, if has the principal projection property, then is a component of if and only if , for some principal projection , Reference 19, Theorem 32.7. If has a weak order unit, say , then is a component of if and only if there is a band projection on with . Further, and for each . We note here that is an module since the -algebra multiplication in is a restriction of that in and if with and then so . Any for which there exist pairwise disjoint components , …, of and real numbers , …, such that is called an -step function. Notice that if has the principal projection property, then there exist principal band projections , …, such that , where the band projections are pairwise disjoint. Consequently, if is a Dedekind complete Riesz space with weak order unit, say , then (where is the principal band generated by ), and any -step function can be represented by .

In order to extend the Koopman-von Neumann Lemma to sequences in a Riesz space, we define a density zero sequence of band projections as follows.

Definition 3.1 (Density zero sequence of band projections).

A sequence of band projections in a Riesz space with weak order unit is said to be of density zero if , in order as .

The above definition could be rephrased as saying that a sequence of components of is said to be of density zero if its Cesàro mean tends to zero in order.

With the above definition of density zero sequences of band projections, we can now give an analogue of the Koopman-von Neumann Lemma in Riesz spaces.

Theorem 3.2 (Koopman-von Neumann).

Let be a Dedekind complete Riesz space with weak order unit, say , and let be an order bounded sequence in the positive cone, , of , then in order, as , if and only if there exists a density zero sequence of band projections on such that , in order, as .

Proof.

Suppose that and there exists with , for all .

If is a density zero sequence of band projections with , in order, as , then

Since is of density zero, in order, as , giving in order, as . Furthermore, by Theorem 2.2, as , in order, as and , we have in order, as . Thus, by Equation 3.1a-Equation 3.1b, as is Archimedean, in order, as .

Conversely, suppose that , in order, as . Let be the band projection onto the band generated by and . Let . Let be the band projection onto the band generated by and . As , we have that . Further, since is increasing in for fixed , it follows that is increasing in for fixed and hence is increasing in for fixed , giving that is increasing in for fixed .

Since it follows that

giving that is decreasing in . Hence, is decreasing in , for fixed . We now show that, for fixed , , in order, as . Since (as is the projection onto the band generated by ), we have

However,

(since is the band projection onto the band generated by ), so, by Equation 3.2 and Equation 3.3, we have

in order, as . Thus, for fixed , , in order, as .

Observe that , since is the band projection onto the band generated by . Let , for , then , say, in order, as . Here, the band projections and can be explicitly determined from their components , for , and , in order, as . Further , , is a partition of for each , that is,

and

in order, as , giving

Let

by Equation 3.5, and in terms of components we have

Further, as , by Equation 3.8,

Hence, subtracting the left-hand side of Equation 3.10 from the right-hand side of Equation 3.10, we obtain

For , , we have that . Now, from the definition of , we have

thus , giving

Hence, Further, , so, for , is in the band generated by , giving Applying the above to , we have

Taking the supremum over in Equation 3.12 gives , since and . Further, , hence, , so multiplying Equation 3.11 by gives

where we have used that . Now, from Equation 3.6, Equation 3.7 and Equation 3.13a-Equation 3.13b, for ,

So, taking the limit supremum as , we obtain

for each . Thus, as is Archimedean, and in order, as .

It now remains to show that in order, as . For and , we have , giving . Thus, for , we have

Summing the above over gives

We recall, from Equation 3.10, that , so if then and , that is, . Hence,

Combining Equation 3.16a-Equation 3.16b and Equation 3.17, we have, for each ,

Here, and both converge, in order, to , so converges to , in order, as , as does . Thus, taking the limit supremum as in Equation 3.18b gives

for each . Hence,

in order, as is Archimedean.

Note 3.3.

If in Theorem 3.2 is not assumed to be order bounded, but in order, as , then it still follows that there is a density zero sequence of band projections, , such that in order, as , but one cannot conclude boundedness of . Further, the converse need not hold. In particular, if is not bounded and there is a density zero sequence of band projections such that in order, as , then one cannot conclude that is order convergent to as .

For example, working in the classical case of , for , we have

is unbounded and is a set of density zero. Here for as but is convergent to for , convergent to a non-zero value for and divergent to for .

4. Application to weak mixing

Let be a probability space, that is, is a set, is a -algebra of subsets of and is a measure on with . The mapping is called a measure preserving transformation if , for each , in which case is called a measure preserving system. Further details may be found in Reference 3Reference 7Reference 14.

The measure preserving system is said to be weakly mixing if

as , for each . To give a Riesz space analogue of a measure preserving system and weak mixing, we recall from Reference 8 the definition of a conditional expectation operator on a Riesz space.

Definition 4.1.

Let be a Riesz space with weak order unit. A positive order continuous projection , with range, , a Dedekind complete Riesz subspace of , is called a conditional expectation operator if is a weak order unit of for each weak order unit of .

If is a conditional expectation operator on with , then is also a conditional expectation operator on , since, if , then , giving .

The Riesz space analogue of a measure preserving system is introduced in the following definition.

Definition 4.2.

Let be a Dedekind complete Riesz space with weak order unit, say, , and be a conditional expectation operator on with . If is an order continuous Riesz homomorphism on with and for each band projection on , then is called a conditional expectation preserving system.

By Freudenthal’s Spectral Theorem, see Reference 19, Theorem 33.2, the condition for each band projection on in the above definition is equivalent to for all . In Reference 9, Theorems 3.7 and 3.9 various generalisations of Birkhoff’s ergodic theorem to conditional expectation preserving systems were given, resulting in convergence conditions for .

We are now in a position to define conditional weak mixing on a Riesz space with a conditional expectation operator and weak order unit.

Definition 4.3 (Conditional weak mixing).

The conditional expectation preserving system is said to be conditionally weak mixing if, for all band projections and on ,

in order, as .

We note that for , the band projections on are of the form , for and . Definition 4.3 now gives a conditional weak mixing condition on , conditioned by , for a sub--algebra of . If , then conditional weak mixing coincides with the weak mixing on .

We recall, Reference 19, pg. 49, that if is a Riesz space and converges to , we say that converges to -uniformly for given if for each , there is some such that whenever .

Theorem 4.4.

Given the conditional expectation preserving system , then the following statements are equivalent.

(1)

is conditionally weak mixing.

(2)

For all , we have that

in order, as .

(3)

For each pair of band projections and on , there is a sequence of density zero band projections, in such that

in order, as .

Proof.

(1)(2): Suppose that is conditionally weak mixing. Let be -step functions with and , where and are band projections on and and are real numbers, , , then

in order, as .

By Freudenthal’s Spectral Theorem, Reference 19, Theorem 33.2, can be expressed as -uniform order limits of sequences, say , of -step functions in and there is so that , for all . This implies that , for each . For each there is so that and for each . Hence, and for each . Let and , then

Hence, , for all with , so

for all . By Equation 4.3a-Equation 4.3b, , in order, as , so

for all , implying that , in order.

(2) (1): Choosing and , the result follows directly.

(1)(3): Taking , the result follows from Theorem 3.2.

5. Application to measurable processes

If we consider the Riesz space of equivalence classes of almost everywhere identical functions in , where is a finite measure (the case of -finite is an easy extension of this case), then is a Dedekind complete Riesz space under a.e. pointwise ordering and , the a.e. equivalence class of the constant function with value , is a weak order for . Here the band projections, , on are multiplication by the characteristic functions of measurable sets, i.e., is of the form for . We recall from Reference 1, Lemma 8.17 and Reference 13, pg. 9, Example (ii) that a sequence is order convergent in if and only if a.e. pointwise and there exists for which a.e. for all .

If is a non-negative order bounded sequence in , i.e., a.e. and there exists so that a.e. for all , then, by Theorem 3.2,

if and only if there is a density zero sequence of band projections such that , in order, as , i.e., there is a sequence of measurable sets with

with in order as .

In the above, and , for each , so and are order bounded and thus order convergent if and only if they are a.e. pointwise convergent. Further, Lebesgue’s Dominated Convergence Theorem is applicable. Thus we have the following.

Corollary 5.1.

If is a non-negative sequence in , where is a finite measure, and there exists so that a.e. for all , then as , if and only if there is a sequence of measurable sets with and as . Here the limits can be taken as either a.e. pointwise or in norm.

Proceeding as in Reference 11, Section 5, the conditional weak mixing of Section 4 can be carried over to to give a characterisation of conditional weak mixing in measure spaces.

Mathematical Fragments

Theorem 2.2.

Let be a Dedekind complete Riesz space and a sequence in with , in order, as , then in order, as .

Theorem 3.2 (Koopman-von Neumann).

Let be a Dedekind complete Riesz space with weak order unit, say , and let be an order bounded sequence in the positive cone, , of , then in order, as , if and only if there exists a density zero sequence of band projections on such that , in order, as .

Equation (3.1)
Equation (3.2)
Equation (3.3)
Equation (3.5)
Equation (3.6)
Equation (3.7)
Equation (3.8)
Equation (3.10)
Equation (3.11)
Equation (3.12)
Equation (3.13)
Equation (3.16)
Equation (3.17)
Equation (3.18)
Definition 4.3 (Conditional weak mixing).

The conditional expectation preserving system is said to be conditionally weak mixing if, for all band projections and on ,

in order, as .

Theorem 4.4.

Given the conditional expectation preserving system , then the following statements are equivalent.

(1)

is conditionally weak mixing.

(2)

For all , we have that

in order, as .

(3)

For each pair of band projections and on , there is a sequence of density zero band projections, in such that

in order, as .

Equation (4.3)

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Article Information

MSC 2020
Primary: 46A40 (Ordered topological linear spaces, vector lattices), 47A35 (Ergodic theory of linear operators), 37A25 (Ergodicity, mixing, rates of mixing), 60F05 (Central limit and other weak theorems)
Keywords
  • Cesàro mean
  • Koopman-von Neumann condition
  • order convergence
  • Riesz spaces
  • conditional expectation operators
  • weak mixing.
Author Information
Jonathan Homann
School of Mathematics, University of the Witwatersrand, Private Bag 3, P.O. WITS 2050, South Africa
jmhomann@gmail.com
ORCID
Wen-Chi Kuo
School of Mathematics, University of the Witwatersrand, Private Bag 3, P.O. WITS 2050, South Africa
wen.kuo@wits.ac.za
MathSciNet
Bruce A. Watson
School of Mathematics, University of the Witwatersrand, Private Bag 3, P.O. WITS 2050, South Africa
b.alastair.watson@gmail.com
ORCID
MathSciNet
Additional Notes

This research was supported in part by the Centre for Applicable Analysis and Number Theory and by National Research Foundation of South Africa grant IFR170214222646 with grant no. 109289.

Communicated by
Stephen Dilworth
Journal Information
Proceedings of the American Mathematical Society, Series B, Volume 8, Issue 7, ISSN 2330-1511, published by the American Mathematical Society, Providence, Rhode Island.
Publication History
This article was received on , revised on , and published on .
Copyright Information
Copyright 2021 by the authors under Creative Commons Attribution-Noncommercial 3.0 License (CC BY NC 3.0)
Article References
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  • DOI 10.1090/bproc/75
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  • Show rawAMSref \bib{4214338}{article}{ author={Homann, Jonathan}, author={Kuo, Wen-Chi}, author={Watson, Bruce}, title={A Koopman-von Neumann type theorem on the convergence of Ces\`{a}ro means in Riesz spaces}, journal={Proc. Amer. Math. Soc. Ser. B}, volume={8}, number={7}, date={2021}, pages={75-85}, issn={2330-1511}, review={4214338}, doi={10.1090/bproc/75}, }

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