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The von Neumann ergodic theorem (the Hilbert space version of the mean ergodic theorem) asserts that if is a unitary operator on a Hilbert space
, and
is a vector in that Hilbert space, then one has
in the strong topology, where is the
-invariant subspace of
, and
is the orthogonal projection to
. (See e.g. these previous lecture notes for a proof.) The same proof extends to more general amenable groups: if
is a countable amenable group acting on a Hilbert space
by unitary transformations
, and
is a vector in that Hilbert space, then one has
for any Følner sequence of
, where
is the
-invariant subspace. Thus one can interpret
as a certain average of elements of the orbit
of
.
I recently discovered that there is a simple variant of this ergodic theorem that holds even when the group is not amenable (or not discrete), using a more abstract notion of averaging:
Theorem 1 (Abstract ergodic theorem) Let
be an arbitrary group acting unitarily on a Hilbert space
, and let
be a vector in
. Then
is the element in the closed convex hull of
of minimal norm, and is also the unique element of
in this closed convex hull.
Proof: As the closed convex hull of is closed, convex, and non-empty in a Hilbert space, it is a classical fact (see e.g. Proposition 1 of this previous post) that it has a unique element
of minimal norm. If
for some
, then the midpoint of
and
would be in the closed convex hull and be of smaller norm, a contradiction; thus
is
-invariant. To finish the first claim, it suffices to show that
is orthogonal to every element
of
. But if this were not the case for some such
, we would have
for all
, and thus on taking convex hulls
, a contradiction.
Finally, since is orthogonal to
, the same is true for
for any
in the closed convex hull of
, and this gives the second claim.
This result is due to Alaoglu and Birkhoff. It implies the amenable ergodic theorem (1); indeed, given any , Theorem 1 implies that there is a finite convex combination
of shifts
of
which lies within
(in the
norm) to
. By the triangle inequality, all the averages
also lie within
of
, but by the Følner property this implies that the averages
are eventually within
(say) of
, giving the claim.
It turns out to be possible to use Theorem 1 as a substitute for the mean ergodic theorem in a number of contexts, thus removing the need for an amenability hypothesis. Here is a basic application:
Corollary 2 (Relative orthogonality) Let
be a group acting unitarily on a Hilbert space
, and let
be a
-invariant closed subspace of
. Then
and
are relatively orthogonal over their common subspace
, that is to say the restrictions of
and
to the orthogonal complement of
are orthogonal to each other.
Proof: By Theorem 1, we have for all
, and the claim follows. (Thanks to Gergely Harcos for this short argument.)
Now we give a more advanced application of Theorem 1, to establish some “Mackey theory” over arbitrary groups . Define a
-system
to be a probability space
together with a measure-preserving action
of
on
; this gives an action of
on
, which by abuse of notation we also call
:
(In this post we follow the usual convention of defining the spaces by quotienting out by almost everywhere equivalence.) We say that a
-system is ergodic if
consists only of the constants.
(A technical point: the theory becomes slightly cleaner if we interpret our measure spaces abstractly (or “pointlessly“), removing the underlying space and quotienting
by the
-ideal of null sets, and considering maps such as
only on this quotient
-algebra (or on the associated von Neumann algebra
or Hilbert space
). However, we will stick with the more traditional setting of classical probability spaces here to keep the notation familiar, but with the understanding that many of the statements below should be understood modulo null sets.)
A factor of a
-system
is another
-system together with a factor map
which commutes with the
-action (thus
for all
) and respects the measure in the sense that
for all
. For instance, the
-invariant factor
, formed by restricting
to the invariant algebra
, is a factor of
. (This factor is the first factor in an important hierachy, the next element of which is the Kronecker factor
, but we will not discuss higher elements of this hierarchy further here.) If
is a factor of
, we refer to
as an extension of
.
From Corollary 2 we have
Corollary 3 (Relative independence) Let
be a
-system for a group
, and let
be a factor of
. Then
and
are relatively independent over their common factor
, in the sense that the spaces
and
are relatively orthogonal over
when all these spaces are embedded into
.
This has a simple consequence regarding the product of two
-systems
and
, in the case when the
action is trivial:
Lemma 4 If
are two
-systems, with the action of
on
trivial, then
is isomorphic to
in the obvious fashion.
This lemma is immediate for countable , since for a
-invariant function
, one can ensure that
holds simultaneously for all
outside of a null set, but is a little trickier for uncountable
.
Proof: It is clear that is a factor of
. To obtain the reverse inclusion, suppose that it fails, thus there is a non-zero
which is orthogonal to
. In particular, we have
orthogonal to
for any
. Since
lies in
, we conclude from Corollary 3 (viewing
as a factor of
) that
is also orthogonal to
. Since
is an arbitrary element of
, we conclude that
is orthogonal to
and in particular is orthogonal to itself, a contradiction. (Thanks to Gergely Harcos for this argument.)
Now we discuss the notion of a group extension.
Definition 5 (Group extension) Let
be an arbitrary group, let
be a
-system, and let
be a compact metrisable group. A
-extension of
is an extension
whose underlying space is
(with
the product of
and the Borel
-algebra on
), the factor map is
, and the shift maps
are given by
where for each
,
is a measurable map (known as the cocycle associated to the
-extension
).
An important special case of a -extension arises when the measure
is the product of
with the Haar measure
on
. In this case,
also has a
-action
that commutes with the
-action, making
a
-system. More generally,
could be the product of
with the Haar measure
of some closed subgroup
of
, with
taking values in
; then
is now a
system. In this latter case we will call
-uniform.
If is a
-extension of
and
is a measurable map, we can define the gauge transform
of
to be the
-extension of
whose measure
is the pushforward of
under the map
, and whose cocycles
for
are given by the formula
It is easy to see that is a
-extension that is isomorphic to
as a
-extension of
; we will refer to
and
as equivalent systems, and
as cohomologous to
. We then have the following fundamental result of Mackey and of Zimmer:
Theorem 6 (Mackey-Zimmer theorem) Let
be an arbitrary group, let
be an ergodic
-system, and let
be a compact metrisable group. Then every ergodic
-extension
of
is equivalent to an
-uniform extension of
for some closed subgroup
of
.
This theorem is usually stated for amenable groups , but by using Theorem 1 (or more precisely, Corollary 3) the result is in fact also valid for arbitrary groups; we give the proof below the fold. (In the usual formulations of the theorem,
and
are also required to be Lebesgue spaces, or at least standard Borel, but again with our abstract approach here, such hypotheses will be unnecessary.) Among other things, this theorem plays an important role in the Furstenberg-Zimmer structural theory of measure-preserving systems (as well as subsequent refinements of this theory by Host and Kra); see this previous blog post for some relevant discussion. One can obtain similar descriptions of non-ergodic extensions by working relative to the invariant factor (or via the ergodic decomposition, if one has enough separability hypotheses on the system), but the result becomes more complicated to state, and we will not do so here; see this paper of Austin for details.
The last two lectures of this course will be on Ratner’s theorems on equidistribution of orbits on homogeneous spaces. Due to lack of time, I will not be able to cover all the material here that I had originally planned; in particular, for an introduction to this family of results, and its connections with number theory, I will have to refer readers to my previous blog post on these theorems. In this course, I will discuss two special cases of Ratner-type theorems. In this lecture, I will talk about Ratner-type theorems for discrete actions (of the integers on nilmanifolds; this case is much simpler than the general case, because there is a simple criterion in the nilmanifold case to test whether any given orbit is equidistributed or not. Ben Green and I had need recently to develop quantitative versions of such theorems for a number-theoretic application. In the next and final lecture of this course, I will discuss Ratner-type theorems for actions of
, which is simpler in a different way (due to the semisimplicity of
, and lack of compact factors).
We continue our study of basic ergodic theorems, establishing the maximal and pointwise ergodic theorems of Birkhoff. Using these theorems, we can then give several equivalent notions of the fundamental concept of ergodicity, which (roughly speaking) plays the role in measure-preserving dynamics that minimality plays in topological dynamics. A general measure-preserving system is not necessarily ergodic, but we shall introduce the ergodic decomposition, which allows one to express any non-ergodic measure as an average of ergodic measures (generalising the decomposition of a permutation into disjoint cycles).
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