C OMPOSITIO M ATHEMATICA
C HARLES P UGH M ICHAEL S HUB
Ergodic elements of ergodic actions
Compositio Mathematica, tome 23, n
o1 (1971), p. 115-122
<http://www.numdam.org/item?id=CM_1971__23_1_115_0>
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115
ERGODIC ELEMENTS OF ERGODIC ACTIONS by
Charles
Pugh
* and Michael Shub **Wolters-Noordhoff Publishing Printed in the Netherlands
1. Introduction
A
question naturally arising
indynamical systems
is: does a flow{~t}
have the same
nonwandering
set as most of the time t maps,ç)
This andsimilar
questions
for recurrency(Poisson stability)
we are unable toanswer. For
ergodicity, however, representation theory of S1
and Stone’s theorem lead to an affirmative answer:If
{~t}
is anergodic
flow then each map qJt,except
for a countable set oft-values,
isergodic (See §
2 fordefinitions).
The
proof of this
wassupplied
to usby
J. Auslander andParthasarathy.
In this paper we ask the
corresponding question
for group actions andanswer it
completely
in the case ofRk-actions. (For
other group actionswe have
partial
results and somecounter-examples).
Theanalysis
is notdiScult.
We
employ
therepresentation theory
ofseparable locally compact
abelian groups, and it seemsstrange
that suchsimple
facts wereapparent- ly
unknown to theergodic
theorists. Ouranalysis
ofRk-actions, k ~ 1,
uses the characterization of
cyclic representations
not Stone’stheorem,
as can be found in
[2].
We are indebted to R. Palais and H. Levine for conversationsleading
to theproof
of the theorem and to W.Parry
forour interest in
ergodic theory.
2. Definitions and the main result
Let G be a group and
(M, Il)
a measure space. An action of G on(M, Il)
is ahomomorphism
p : G - Auto(M, 03BC).
The elements of Auto(M, Il)
are the measurablebijections
of M onto itself with measurableinverses. If G has a
topology,
thehomomorphism
p isrequired
to becontinuous in the sense that
* Supported by the sloan Foundation and NSF GP8007.
** Nato Postdoctoral fellow.
116
be continuous. We shall denote the
operator
onL2(M, 03BC), f ~ f
pg,as p* g.
The action p : G ~ Auto
(M, Il)
is said to beergodic
iff1.
p(g)
ismeasure-preserving
foreach g
E G.2.
If f ~ L2(M, p)
is invariant(i.e. 03C1*(g)f
=f for each g
EG) then f is
constant.
As is
standard, ’equal’
means’equal
almosteverywhere’
and ’constant’means
’equal
to a constant-function almosteverywhere’.
In terms ofp* : le means that p* : G ~
Un(L2(M, 03BC)),
theunitary operators
onL2(M, y).
An
element g
of G is said to beergodic
if pg is measurepreserving
and 03C1*g has
cnly
constant invariant functions.We are interested in
knowing
when anergodic
action hasergodic
elements without much restriction on
(M, Jl)
or p. We haveproved
thefollowing
THEOREM 1.
If Rk
actsergodically
on(M, 03BC), M(M)
oo, andL2 (M, y)
is
separable,
then all the elementsof Rk, off
a countableof family hyper- planes,
areergodic.
When we
speak
ofplanes, lines,
etc., we do not assume thatthey
contain the
origin.
A moregeneral
group is discussed in§
6.Rk acts
onitself naturally by
translation03C1(g) : y
H y + g.Factoring by zk gives
the natural actionof Rk
onTk,
the k-torus. Theorem 1generalizes
the fact that under this natural action every element
of Rk, off a
countablefamily
ofhyperplanes,
actsergodically
onT .
In this case we canidentify
the
hyperplanes
as thosepoints y
ERk whose components
y 1, ..., yk arerationally dependent. Unfortunately
we can’tgive
such a neat determina-tion of the
non-ergodic
elements for ageneral
action ofRk.
As some of our work is valid for groups G more
general
thanRk,
we shallonly
assumeabelian Hausdorff
G is
locally compact separable 03BC(M)
~L2 (M, li) separable
p : G - Auto
(M, p)
isergodic.
We recall that a
unitary representation
of G is ahomomorphism r sending
G into the group ofunitary operators
on someseparable
Hilbertspace H.
Continuity
of(g, h)
H(rg)(h)
isrequired.
Then p* : G -Un(L2(M, Jl»
is aunitary representation
of G.3.
Cyclic representations
The
representation r :
G -Un(H)
iscyclic
if there is a nonzero vectorv E H such that the
only
closedsubspace
of Hcontaining
the orbitof v,
{(rg)(v) : g
EG}
is H itself. To anycyclic representation r :
G -Un(H)
there
corresponds
aunique
normalized Borelmeasure p
on the character group,6 = Hom(G, S1),
such that r isunitarily equivalent
to the’direct
integral’ representation m :
G -Un(L2(G, 03B2))
definedby
See
[2].
Thus for afixed g
EG,
we have theunitary operator L2(, 03B2)
~L2(G, 03B2)
definedby m(g) f H ·, g>f(·).
Now let us return to the
ergodic
action p : G -Auto(M, Il)
and theinduced
unitary representation
p* : G ~Un(M, 03BC).
The spaceL2(M, 03BC)
may be written as the countable direct sum
(of orthogonal
closed sub-spaces)
where C is the one dimensional space of constant functions and 03C1* G is
a
cyclic representation
onHi.
That is each p* g leavesHi
invariant and(restriction
toHi)
o p* : G -Hi
iscyclic.
For inC~
we choose any vectorV ~
0 and look atHi,
the smallest closedsubspace of L2(M, Il)
containing
its orbit. As p* is aunitary representation,
it leavesCl
invariant and so
Hi 1
C. SinceL2(M, Il)
isseparable (by assumption)
Zorn’s lemma lets us
proceed inductively
to define such an invariantsplitting
C E9Hl
E9H2 ~ ···
=L2(M, y).
Let us write p*i
for (restriction
toHi)
o p* : G -Hi.
For each i the
representation
03C1*i isunitarily equivalent
to the directintegral representation
mi onL2(G, Pi)
for someunique
normalizedBorel
measure Plon G ;
m i : G ~Un(L2 (G, 03B2i))
definedby
LEMMA 1.
If
e is theidentity
elementof G
then 8 has zerof3i-measure for
each i.PROOF. If
Pi(8)
> 0 then let E be the characteristic function of 8. InL2(, 03B2i), E ~
0 because03B2i(03B5) ~
0. But(m i g)E = ·, g> E(.)
andevaluated on any v E
G
this isThus
(mig)E
= E forall g
E G and so E would be a nonzero invariantvector for all the
operators
mig. But the inverse of theconjugacy
118
hi : Hi --+ L2(, 03B2i)
carries E on toh-1i(E),
a nonzero invariant vectorof p* i . Since
h-1i(E)
lies inHi
andHi-1. C, h-1i(E)
is nonconstant.Thus p* has a nonconstant invariant function in
L2(M, y), contradicting
the fact that p is
ergodic.
Hence03B2i(03B5)
=0, proving
the lemma.For any g E G let
and for any x E
G
let4. A criterion for non
ergodicity
The next lemma
distinguishes
thoseelements g
E G which are notergodic.
LEMMA 2.
If go E G is
not anergodic
elementfor
the action p then03B2i(ker g0) > 0 for
some i.PROOF. That go is not
ergodic
means p* go :L2(M, 03BC) ~ L2(M, 03BC)
has a nonconstant invariant
function,
say w. The invariantcyclic
de-composition L2(M, 11)
= C(Di i Hi gives w
= c+Zi
wi andwi ~
0 forsome i. Then w, is a nonzero invariant vector of p* go
lying in Hi.
Thatis,
wi is a nonzero invariant vector of 03C1*ig0, the restriction of p* go toHi.
But p*is cyclic
and so isconjugate
to therepresentation
mi : G ~Un(L’(0, 03B2i))
definedby
The
conjugacy hi
makescommute. The
conjugate
of wi,hi W = f,
is a nonzero invariant vectorof mig0. But since we know the formula
defining
mig0, this says thatin
L2(G, 03B2i). Since f ~
0 inL2(, 03B2i),
the factor1- y, g0>
vanishes ona set of
positive 03B2i-measure.
That is{~
E0 : ~, g0> = 1}
= ker go haspositive 03B2i-mesaure.
As an immediate
corollary
we havePROPOSITION. The
ergodic
action p has(a)
someergodic elements, if
G is not the unionof
its proper closedsubgroups
(b) a
Baire setof ergodic
elementsif
G iscompact
and every proper closedsubgroup
is nowhere dense(c) a
contralinear Baire setof ergodic
elementsif
G =Tk.
PROOF.
If g E G is
nonergodic
then03B2i(ker g)
> 0 for some i andker g
contains a nonzero element x,
by
Lemma1,
so g E ker(X).
This ker X is a proper closedsubgroup
of G.(a)
Fromthis, (a)
is clear.(b)
If G iscompact, 6
is countable[3]
and so eachnonergodic g
E Gis contained in some ker
(x)
where x ranges over a countable set. Thecountable union of these nowhere dense
subsets,
ker(x),
includes allnon
ergodic
elements and itscomplement
is the asserted Baire set.(c)
If G isTk then
each ker(x)
is ahyperplane
for x E= Zk.
By
contralinear we mean thecomplement
of thefamily
ofrationally dependent
sub-tori.REMARK. For
(b), (c)
we did not have to use the characterization of acyclic representation,
since in thecompact
case we maydecompose
p*into a direct sum of
irreducible,
1-dimensionalrepresentations.
5. G
= Rk
and theproof
of Theorem 1Now we shall let G
= Rk. Since Rk - Rk,
we shall beworking
withnormalized Borel
measures P
onRk.
For anysuch P
letf!JJ 0 =
the set ofpoints
P ERk with 03B2(P)
> 0.Pn =
the set ofn-planes
P cRk
with03B2(P)
> 0 butcontaining
noelement of
Pm, m
n.This makes
’9k+ 1
=0. Let P
=P0
~ ... uPk.
LEMMA 3. É9 is at most countable.
PROOF. If
P,
P’ Ef!JJn
are not identical then03B2(P
nP’)
= 0 sinceP n P’ is a lower dimensional
plane
in each.Thus,
ifP1, ···, Pm
Ef!JJ n
are distinct then
Since
03B2(Rk)
= 1 there can therefore be no more than mplanes
P eY.
120
having measure 1/m. Letting
m - oo we exhaust all ofPJJn by
finitesets;
hence Y
is at most countable.As remarked
before, Rk
is it own character group wherex, y) = e21ty(x,y)
and(x, y) is
the usual dotproduct
inRk; (We
thinkalways
ofx ~ = Rk, y ~ G = Rk).
Thenker (x) = {y ~ Rk : x,y> = 1} = {y ~ Rk : (x, y) ~ Z} .
LEMMA 4.
I,f’ 03B2(0)
= 0 and B ={y
ERk : 03B2(ker y)
>01
then B iscontained in
countably
manyhyperplanes.
PROOF. Since
03B2(ker y)
>0, ker y
must contain an element P of Y andsince
03B2(0)
= 0 such aP ~
0 may be chosen. All the elements x ~ P have y in theirkernels;
that is x ~ker y « y
E ker x. Hence foreach y
E Bthere exists P E PJJ such
that y
EnxEP-0
ker x. Since P ranges over thecountable set
PJJ, independant of y
EB,
the lemma isproved.
PROOF oF THEOREM 1. For each normalized Borel measure
03B2i on Rk
asabove,
the setBi
given in lemma 4 is contained incountably
manyhyper- planes.
For03B2i(0)
= 0 is satisfiedby
Lemma 1.By
Lemma2, if y ~ Rk
isnot
ergodic then y
EBi
for some i and the theorem isproved.
Now we
give examples
of some groups which can actergodically
without
having
anyergodic
elements.EXAMPLE 1. Give the rationals
Q
the discretetopology
and let p :Q -
Auto(S1, d03B8)
be definedby
rotationThe action is
ergodic
becauseif f were
a nonconstant invariant function for all theoperators p*(p/q)
it would be anL2
function which wasperiod-
ic of every rational
period.
Suchan f cannot
existby taking
its Fourierexpansion. However,
each03C1*(p/q)
has invariant functionse2"it
He2niqmt
m
being
anypositive integer.
EXAMPLE 2.
Let m ~
2 and n ~ 1 beintegers
and let k = mn. LetG =
Z.
@Zk
and M =Z.
0Zm .
Define p : G ~Auto(M, 11) by
where + is taken in
Z.
and t’ is first reduced mod m. The measure yon
Zm
(DZ. equals 11m2
on eachpoint.
The action p isergodic
becausein fact it is transitive.
However,
for any g =(t, t’)
E G there is an in-variant function for p*g which is the characteristic function
f,
ofT =
{(t, t’), (2t, 2t’), ···, (mt, mt’)} ~
M. The set T is invariantby
pg,so its characteristic function is invariant
by
p* g. Since T has m elements and M hasm2 elements, , f is
non constnat inL2(M, 03BC).
In
example 2, Zm Ee Zk
may bereplaced by
any group Gsurjecting continuously
ontoZm
0Zk:
So if G is of the form
Rk x Tn
x F when Fis afinitely generated
abeliangroup then we have answered the
question
of’ergodicity
~ergodic
elements’
negatively
if F is notcyclic.
The case when F iscyclic easily
reduces to the
study
of G =Rk
xZ,
for which we prove ageneralization
of theorem 1.
THEOREM 2.
If
G =Rk x
Z actsergodically
on(M, Il)
then all elements g ERk {1}, off a
countable unionof hyperplanes
inRk {1},
areergodic.
Since any Abelian Lie group
generated by
acompact neighborhood
ofthe
identity
can beexpressed Rk x Tn
x F where F is afinitely generated
discrete group, Theorems
1,
2 andExample
2 answer thequestion:
whendoes
ergodicity
of the G actionimply
the existence ofergodic
elementsfor such a group G? The
product decomposition
follows from[3 ] and [4].
PROOF oF THEOREM 2. Instead of the
planes
P EPn
consider translates of closed connectedsubgroups
of6
=Rk x S1 having
dimension n,positive 03B2
measure, andcontaining
no elements ofP0 ~···~ Pn-1.
By
the sameargument Y = P0 ~···~ ÇJJk+ 1
is countable.(It
isonly
necessary to observe that the intersection P n P’ has dimension n if
P,
P’ EYn
aredistinct.) If g
ERk {1}
is notergodic
then03B2i(ker g)
> 0 for one of themeasures 03B2i arising
in§ 3.
Since03B2i(03B5)
=0,
there exist P EPi,
P ~ e, P c ker g, and x EP, ~ ~
8, can be chosen. We have x =(x, e203C0i03BE)
with x ~Rk and 0 ~ 03BE
1.Then 9
E ker(x)
andNow
if x ~
0 then it is clear thatRk {1}
n ker x is a countablefamily of hyperplanes.
But if x = 0 then ker(x)
nRk
x{1}
=0 since ç =1=
0 and0 ~ 03BE
1.[Note
that if we haddealt,
with sayRk
x{2}
we would haveconsidered
{(2y, 2) : (x, y)+203BE
EZ}.
If x ~ 0 then this is a countablefamily
ofhyperplanes.
But if x = 0 it ispossible for 03BE
toequal 1/2
andthe set to be all of
Rk
x{2}. ] See
alsoexample
3 below.Since each non
ergodic g
ERk {1} belongs
to a countablefamily
ofhyperplanes ~~~P-03B5
ker(x)
nRk {1}
and these P are chosenalways
122
from the sequence of countable families
P1, P2, ···,
thetotality
ofhyperplanes
necessary to contain{g ~ Rk {1} : g
is notergodic}
is atmost coutable.
EXAMPLE 3. This
example
was shown to usby
K.Sigmund. Ergodicity
of an action p : Z -
Auto(M, p)
isequivalent
toergodicity
ofp( ± 1 ).
Here we observe that
p(n)
may fail to beergodic
for all n other than:t 1.
This shows that our concentration on the
nonergodic
elementlying
inRk {1}
was necessary.Let M =
Z2 Z3 ···
=03A0p~ Zp,
= theprimes.
Let y, be the nor- malized measure onZp, /lp(S)
=cardinality (S)/p
and let 03BC =03A0p~B
mp . This makes(M, p)
a normalized measure space andL2 (M, p) separable.
The action p : Z -
Auto(M, 03BC)
definedby p(n) : (zp)
r+(zp+pn)
isergodic
butp(n)
is notergodic
unless n =±1. Ergodicity
of p follows from some standardergodic theory [1 ].
Nonergodicity of 03C1(n), n ~
±1,
is clear since
p(n)
leaves invariant each ofthe q
sets of measure1/q, S0 = {(Zp) ~ 03A0Zp : zq
=0}, ···, Sq-1 = {(zp)
eHzp : zq
=q-1}
whereq is a
prime dividing
n.REFERENCES
BILLINGSLEY
[1] Ergodic Theory and Information. John Wiley and Sons. New York, 1965, p. 17.
G. W. MACKEY
[2] Group representations and Applications. Lectures given at Oxford University, 1966-1967.
L. PONTRIJAGIN
[3] Topological Groups. Princeton University Press.
A. WEIL
[4] L’integration dans les Groupes Topologiques et ses applications .Hermann, Paris (1951).
(Oblatum 22-V-1970) Institut des Hautes Etudes Scientifiques,
91 - Bures-sur-Yvette.
Prof. C. Pugh Prof. M. Shub
Department of Mathematics Department of Mathematics University of California Brandeis University BERKELEY, Calif. 94720 WALTHAM, Mass. 02154
U.S.A. U.S.A.