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EXACTNESS OF ROKHLIN ENDOMORPHISMS
AND WEAK MIXING OF POISSON BOUNDARIES.
& MARIUSZ LEMANCZYK
JON AARONSON
ABSTRACT. We give conditions for the exactness of Rokhlin endomorphisms, apply
these to random walks on locally compact, second countable topological groups and
obtain that the action on the Poisson boundary of an adapted random walk on such
a group is weakly mixing.
§
0 INTRODUCTION
Rokhlin endomorphisms.
By a
non-singular endomorphism
we mean a quadruple (
X,B,m,T
) where
(
X,B,m
) is a standard probability space and
T
:
X
0
→X
0
is a measurable trans-
formation of
X
0
∈B, m
(
X
0
) = 1 satisfying
m
(
T
−1
A
) = 0
⇔m
(
A
) = 0 (
A∈B
).
As in [Ro2], the endomorphism
T
is called
exact
if
T
(
T
) :=
T
∞
n=0
T
−n
B
=
{∅,X}
.
Let
G
be a locally compact, Polish topological (LCP) group.
By a
non-singular
G
-action
on a probability space (
Y,C,ν
) we mean a measurable
homomorphism
S
:
G→
Aut (
Y
) where Aut (
Y
) denotes the group of invertible,
non-singular transformations of
Y
equipped with its usual Polish topology.
The
action
S
is called
probability preserving
if each
S
g
preserves
ν
.
Given a non-singular endomorphism (
X,B,m,T
), a non-singular
G
-action
S
:
G→
Aut (
Y
) of a LCP group
G
and a measurable function
f
:
X→G
, we consider
the
Rokhlin endomorphism
e
e
T
=
T
f,S
:
X×Y→X×Y
dened by
e
T
(
x,y
) := (
Tx,S
f (x)
y
)
.
Rokhlin endomorphisms rst appeared in [Ro1] (see also [AR]). We give conditions
for their exactness (theorem 2.3).
These conditions are applied to random walk endomorphisms. Meilijson (in
[Me]) gave sucient conditions for exactness for random walk endomorphisms over
G
=
Z
. We clarify Meilijson’s theorem proving a converse (proposition 4.2), extend
it to LCP Abelian groups (theorem 4.1), characterize the exactness of the Rokhlin
endomorphism for a steady random walk (theorem 4.5) and obtain that the group
action on the Poisson boundary (see
§
4) of an adapted (i.e.
globally supported)
random walk is weakly mixing (proposition 4.4).
1991
Mathematics Subject Classication
. 37A20, 37A15 (37A40, 60B15, 60J50).
c
2004. Aaronson was partially supported by the EC FP5, IMPAN-BC Centre of Excellence
when this work was begun. Lemanczyk’s research was partially supported by KBN grant 1 P03A
03826. Both authors thank MPIM, Bonn for hospitality when this work was nished.
Typeset by
A
M
S
-T
E
X
& MARIUSZ LEMA NCZYK
2
JON AARONSON
Tools employed include the ergodic theory of “associated actions” (see
§
1), and
the boundary theory of random walks (see
§
4).
The authors would like to thank the referee for some useful comments including
a simplication in the proof of proposition 3.4.
§
1 ASSOCIATED ACTIONS
For a non-singular endomorphism (
Z,D,ν,R
) set
•I
(
R
) :=
{A∈D
:
R
−1
A
=
A}
– the
invariant
σ
-algebra, and
•T
(
R
) :=
T
∞
n=0
R
−n
D
– the
tail
σ
-algebra.
Let (
X,B,m,T
) be a non-singular endomorphism. Let
G
be a locally compact,
Polish topological (LCP) group, let
f
:
X→G
be measurable.
There are two
associated (right)
G
-actions
arising from the invariant and tail
σ
-algebras of
T
f
, which are dened as follows:
•
dene the (left)
skew product
endomorphism
T
f
:
X×G→X×G
by
T
f
(
x,g
) :=
(
Tx,f
(
x
)
g
) and x
P∈P
(
X×G
)
, P∼m×m
G
;
•
for
t∈G
, dene
Q
t
:
X×G→X×G
by
Q
t
(
x,g
) := (
x,gt
−1
), then
Q
t
◦T
f
=
T
f
◦Q
t
.
The associated invariant action.
The
invariant factor
of (
X×G,B
(
X×G
)
, P,T
f
) is a standard probability space
(
,F,P
) = (
I
,F
I
,P
I
) equipped with a measurable map
π
:
X×G→
such
that
P◦π
−1
=
P, π◦T
f
=
π
and
π
−1
F
=
I
(
T
f
).
Since
Q
t
I
(
T
f
) =
I
(
T
f
) (because
T
f
◦Q
t
=
Q
t
◦T
f
),
•∃
a
P
-non-singular
G
-action
P
:
→
so that
π◦Q
=
P◦π
.
Proposition 1.1.
(
,F,P, P
)
is ergodic i
(
X,B,m,T
)
is ergodic.
Proof.
If (
X,B,m,T
) is ergodic, then so is (
X×G,B
(
X×G
)
, P,T
f
,Q
) where
T
f
,Q
denotes the
Z
+
×G
action dened by (
n,t
)
→T
f
◦Q
t
∈
Aut (
X×G
). Any
P
-invariant, measurable function on lifts by
π
to a
T
f
,Q
-invariant, measurable
function on
X×G
, which is
P
-a.e. constant.
Conversely, any
T
-invariant function on
X
lifts to a
T
f
-invariant function on
X×G
which is also
Q
-invariant and thus the lift of a
P
-invariant, measurable
function on . If (
,F,P,g
) is ergodic this function is constant (a.e.).
€
The non-singular
G
-action (
,F,P, P
) is called the
invariant-
or
Poisson
G
-
action associated to
(
T,f
) and denoted
P
=
P
(
T,f
).
This action is related to the
Mackey range
of a cocycle (see [Zi2] and
§
3), and
the
Poisson boundary
of a random walk (see
§
4).
The associated tail action.
The
tail factor
of (
X×G,B
(
X×G
)
, P,T
f
) is a standard probability space
(
,F,P
) = (
T
,F
T
,P
T
) equipped with a measurable map
π
:
X×G→
such
that
P◦π
−1
=
P, π
−1
F
=
T
(
T
f
).
Since
Q
t
T
(
T
f
) =
T
(
T
f
) (because
T
f
◦Q
t
=
Q
t
◦T
f
),
•∃
a
P
-non-singular
G
-action
τ
:
→
so that
π◦Q
=
τ◦π
.
Proposition 1.2.
(
,F,P,τ
)
is ergodic i
(
X,B,m,T
)
is exact.
Proof.
Suppose rst that (
X,B,m,T
) is exact. Any
τ
-invariant, measurable func-
tion
F
:
→R
lifts by
π
to a
Q
-invariant,
T
(
T
f
)-measurable function
F
:
X×G→
R
. In particular
∃
!
F
n
:
X×G→R
(
n≥
0), measurable so that
F
=
F
n
◦T
n
. It
EXACTNESS
3
follows from
Q
t
◦T
f
=
T
f
◦Q
t
that each
F
n
is
Q
-invariant, whence
∃F
n
:
X→R
measurable so that
F
n
(
x,y
) =
F
n
(
x
) for
P
-a.e. (
x,y
)
∈X×G
. Thus
F
=
F
0
=
F
0
is
T
(
T
)-measurable, whence constant
P
-a.e. by exactness of
T
.
Conversely, any
T
(
T
)-measurable function on
X
lifts to a
T
(
T
f
)-measurable
function on
X×G
which is also
Q
-invariant and thus the lift of a
τ
-invariant, mea-
surable function on . If (
,F,P,τ
) is ergodic this function is constant (a.e.).
€
The non-singular
G
-action (
,F,P,τ
) is called the
associated tail
G
-action
(of
(
T,f
)) and denoted
τ
=
τ
(
T,f
). As with the Poisson action, the tail action is
related to the Mackey range of a cocycle, and also to the
tail boundary
of a random
walk (see
§
4).
§
2 CONDITIONS FOR EXACTNESS AND A CONSTRUCTION OF ZIMMER
We begin with a proposition generalising Zimmer’s construction (in [Zi1]) of
a
G
-valued cocycle over an ergodic, probability preserving transformation with a
prescribed ergodic, non-singular
G
-action as Mackey range.
Proposition 2.1.
Suppose that
G
is a LCP group,
that
(
X,B,m,T
)
is a non-singular endomorphism, and suppose that
f
:
X→G
is
measurable.
Let
S
be a non-singular
G
-action on a probability space
(
Y,C,ν
)
and dene
e
T
=
e
T
f,S
:
X×Y→X×Y
by
e
T
(
x,y
) := (
Tx,S
f (x)
y
);
then
T,f
)
∼
=
P
(
T,f
)
×S,
&
τ
(
e
T,f
)
∼
=
τ
(
T,f
)
×S.
e
P
(
Proof.
Dene
π
:
X×Y×G→X×G×Y
by
π
(
x,y,g
) := (
x,g,S
g
−1
y
)
.
Evidently
π
is a bimeasurable bijection.
Fix
p∈P
(
G
)
, p∼m
G
. A calculation shows that
(
m×ν×p
)
◦π
−1
∼m×p×ν,
(1)
indeed
d
(
m×ν×p
)
◦π
−1
d
(
m×p×ν
)
(
x,g,y
) =
dν◦S
g
dν
(
y
) =:
D
(
g,y
)
.
Next, we claim that
e
(2)
π◦
T
f
= (
T
f
×
Id
|
Y
)
◦π.
To see this,
e
π◦
T
f
(
x,y,g
) =
π
(
Tx,S
f (x)
y,f
(
x
)
g
) = (
Tx,f
(
x
)
g,S
(f (x)g)
−1
S
f (x)
y
)
= (
Tx,f
(
x
)
g,S
−1
y
) =
T
f
×
Id
◦π
(
x,y,g
)
.
& MARIUSZ LEMA NCZYK
4
JON AARONSON
It follows from (2) that
e
e
T
f
) =
π
−1
(
I
(
T
f
×
Id))
,T
(
T
f
) =
π
−1
(
T
(
T
f
×
Id))
.
I
(
Now, in general
I
(
T
f
×
Id) =
I
(
T
f
)
⊗B
(
Y
)
,T
(
T
f
×
Id) =
T
(
T
f
)
⊗B
(
Y
)
mod
m×p×ν
and so
e
e
T
f
) =
π
−1
(
I
(
T
f
)
⊗B
(
Y
))
,T
(
T
f
) =
π
−1
(
T
(
T
f
)
⊗B
(
Y
))
I
(
mod
m×p×ν.
e
e
e
P
i
) (
i
=
P, τ
) be the invariant or tail factors
of (
X×G,m×p,T
f
) and (
X×Y×G,m×ν×p,
Now let (
i
,F
i
,P
i
) and let (
i
,
F
i
,
e
T
f
) respectively, according to
the value of
i
=
P, τ
. By (1) and (2),
π
induces a measure space isomorphism of
(
e
e
i
,
P
i
) with (
i
×Y,P
i
×ν
).
Denoting the associated
G
-actions by
e
Q
t
(
x,y,g
) := (
x,y,gt
−1
) and
Q
t
(
x,g
) :=
(
x,gt
−1
), we note that
e
Q
t
= (
Q
t
×S
t
)
◦π.
The proposition now follows from this.
π◦
€
Corollary 2.2.
1)
e
T
is ergodic i
P
(
T,f
)
×S
is ergodic.
e
2)
T
is exact i
τ
(
T,f
)
×S
is ergodic.
3) If both
T
f
and
S
are ergodic, then
e
T,f
)
∼
=
S.
e
T
is ergodic and
P
(
T,f
)
∼
=
S.
Proof.
Parts 1) and 2) follow from propositions 1.1 and 1.2. Parts 3) and 4) follow
from these and form essentially Zimmer’s construction.
e
e
4) If
T
f
is exact and
S
is ergodic, then
T
is exact and
τ
(
€
§
3 LOCALLY INVERTIBLE ENDOMORPHISMS
In this section, we obtain additional results for a non-singular, exact endomor-
phism (
X,B,m,T
) of a standard measure space which is
locally invertible
in the
sense that
∃
an at most countable partition
α⊂B
so that
T
:
a→Ta
is invertible,
non-singular
∀a∈α
. Under the assumption of local invertibility, the associated
actions of
§
1 are
Mackey ranges of cocycles
(as in [Zi2]). See proposition 3.2 (below).
As in [S-W], we call an ergodic, non-singular
G
-action (
X,B,m,U
)
properly er-
godic
if
m
(
U
G
(
x
)) = 0
∀x∈X
and call a properly ergodic, non-singular
G
-action
S
:
G→
Aut (
Y
)
mildly mixing
if
U×S
is ergodic for any properly ergodic
non-singular
G
-action (
X,B,m,U
). As shown in [S-W]:
•
there are no mildly mixing actions of compact groups,
•
a mildly mixing action of non-compact LCP group has an equivalent, invariant
probability. Moreover,
•
a probability preserving
G
-action (
G
a non-compact LCP group) (
Y,C,ν,S
) is
mildly mixing i
L
2
(ν)
−→f⇒f
is constant
.
G
−→∞, f◦S
g
N
f∈L
2
(
ν
)
, g
n
∈G, g
n
We prove
EXACTNESS
5
Theorem 3.1.
Suppose that
(
X,B,m,T
)
is a non-singular, locally invertible, exact endomor-
phism of a standard measure space, that
G
is a LCP, non-compact, Abelian group
and that
f
:
X→G
is measurable.
Either
e
T
f,S
is exact for every mildly mixing probability preserving
G
-action
S
:
G→
Aut (
Y
)
, or
∃
a compact subgroup
K≤G, t∈G
and
f
:
X→K, g
:
X→G
measurable so that
f
=
g−g◦T
+
t
+
f.
Note that the invertible version of this generalizes corollary 6 of [Ru]. The rest
of this section is the proof of theorem 3.1.
Tail relations.
Let (
X,B,m,T
) be a non-singular, locally invertible endomorphism of a standard
probability space. Consider the
tail relations
T
(
T
) :=
{
(
x,y
)
∈X×X
:
∃k≥
0
, T
k
x
=
T
k
y}
;
G
(
T
) :=
{
(
x,y
)
∈X
0
×X
0
:
∃k, ℓ≥
0
, T
k
x
=
T
ℓ
y}
where
X
0
:=
{x∈X
:
T
n+k
x
=
T
k
x∀n, k≥
1
}
. We assume that
m
(
X\X
0
) = 0
(which is the case if
T
is ergodic and
m
is non-atomic) and so
T
(
T
)
⊂G
(
T
)
mod
m
. Both
T
(
T
) and
G
(
T
) are
standard, countable,
m
-non-singular equivalence
relations
in sense of [F-M] whose invariant sets are given by
I
(
G
(
T
)) =
I
(
T
)
, I
(
T
(
T
)) =
T
(
T
)
respectively.
Given a LCP group
G
and
f
:
X→G
measurable, dene
f
n
:
X→G
(
n≥
1)
by
f
n
(
x
) :=
f
(
T
n−1
x
)
f
(
T
n−2
x
)
...f
(
Tx
)
f
(
x
)
and dene
f
:
G
(
T
)
→G
by
f
(
x,x
′
) :=
f
ℓ
(
x
′
)
−1
f
k
(
x
) for
k, ℓ≥
0 such that
T
k
x
=
T
ℓ
x
′
(this does not depend on the
k, ℓ≥
0 such that
T
k
x
=
T
ℓ
x
′
for
x,x
′
∈X
0
).
It follows that
f
:
G
(
T
)
→G
is a (left)
G
(
T
)
-orbit cocycle
in the sense that
f
(
y,z
)
f
(
x,y
) =
f
(
x,z
)
∀
(
x,y
)
,
(
y,z
)
∈G
(
T
)
.
Note that since
T
(
T
)
⊂G
(
T
)
mod
m
, the restriction
f
:
T
(
T
)
→G
is a (left)
T
(
T
)-orbit cocycle.
Mackey ranges of cocycles. Let
R
be a countable, standard, non-singular equiv-
alence relation on the standard measure space (
X,B,m
) and let
:
R→G
be a
left
R
-orbit cocycle. It follows from theorem 1 in [F-M], there is a countable group
and a non-singular -action (
X,B,m,V
) so that
R
=
R
V
:=
{
(
x,V
γ
x
) :
γ∈
, x∈X}.
Let
f
(
γ,x
) := (
x,V
γ
x
) (
f
=
f
,V
:
×X→G
) be the associated
left
V
-cocycle
(satisfying
f
(
γγ
′
,z
) =
f
(
γ,V
γ
′
z
)
f
(
γ
′
,z
)).
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