A NNALES DE L ’I. H. P., SECTION B
M ICHAEL T. L ACEY
The return time theorem fails on infinite measure-preserving systems
Annales de l’I. H. P., section B, tome 33, n
o4 (1997), p. 491-495
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491
The return time theorem fails
on
infinite measure-preserving systems
Michael T. LACEY Georgia Institute of Technology,
Atlanta, GA 30332 USA.
E-Mail: lacey@math.gatech.edu
Vol. 33, n° 4, 1997, p. -495. Probabilités et Statistiques
ABSTRACT. - The Return Time Theorem of
Bourgain [BFKO]
cannot beextended to the infinite
measure-preserving
case.Specifically,
there exista
sigma-finite measure-preserving system (X, A,
~,T)
and a set A c Xof
positive
finite measure so that for almost every xE X
thefollowing
undesirable behavior occurs. For every
aperiodic measure-preserving system
(Y, B,
v,S),
withv (S)
=1,
there is asquare-integrable g
on Y sothat the averages
diverge
a.e.(y),
whereTn
=7-.~) = ~m-1 lA (Tn x).
RESUME. - Le theoreme du
temps
de retour deBourgain
nepeut
pas etre etendu au cas des transformationspreservant
une mesureinfinie. Precisement il existe un
systeme preservant
une mesurea-finite,
(X, A, p, T)
et un ensemble A c X de mesurepositive
etfinie,
telsque pour presque tout x
E X,
on a lecomportement
indesirable suivant.Pour
chaque systeme preservant
la mesureaperiodique (Y, B,
v,S),
avecv (S)
=1,
il existe unefonction g
de carreintegrable
sur Y telle que les moyennesX~~=i lA (Tm x) g y) divergent
pour presque tout(y) ,
Tn
(x) _ ~m-1 lA (Tn x).
Consider an
ergodic measure-preserving system (X, A,
~T). Initially
assume +00; for a set A c X of
positive
measure and xE X
fixed consider the return times =
{7Z
> 0 : E~4}
of the orbit x, Annales de l’lnstitut Henri Poincaré - Probabilités et Statistiques - 0246-0203Vol. 33/97/04/$ 7.00/© Gauthier-Villars
492 M. T. LACEY
T x, T 2 x,
... to the set A. These sets ofintegers
have a rich arithmeticalstructure in both a mean and
pointwise
sense. We are interested in thelatter,
and inparticular
inusing
the return times as sets ofintegers along
which to form new
ergodic
theorems. Theergodic
theorem itselfimplies
that
Nx
hasdensity (A)
for a.e. x. the Wiener-Wintner Theorem[WW]
goes
further, asserting
that anL2 ergodic
theorem holdsalong
for a.e.x, for all second
systems (Y, B, v, S) and g
EL2 (Y)
converges in
L2 (Y).
The much more recent Return Time Theorem ofBourgain [BFKO] strengthens
converge topointwise
in Y. This is a very delicate result.The form of these last two theorems is to consider sets of
integers arising
from a
"timing system" X and, pointwise
inX,
establish a result valid forall "test
systems"
Y. We pose thequestion
ofreplacing
thetiming system
Xby
asigma-finite measure-preserving system,
while stillrequiring
thetest
systems
to be finite. The effect of thischange
on the Wiener-Wintner and Return Time theorems is dramatic. It appears that aninteresting
formof the first theorem could be true, but it can no
longer
be seen from asimple weak-convergence principle,
as is illustrated in[BL,
section2].
Butthe Return Time Theorem in this new formulation is false. This note
gives
a
proof
of the result stated in the abstract. It will follow fromPROPOSITION. - Let
Xm
benon-negative
i.i.d.integer-valued
randomvariables such that P
(Xl> ~) ~
+0o. Here 0 a1,
so that
EX1
= +0oo. Then withprobability 1, for
everyaperiodic finite measure-preserving
system(Y, B,
v,S)
there is asquare-integrable function
g on Y
for
whichwhere the power
of
S above is Tn =~m=1 Xm.
It is well known that Tm can be realized as the return times to the base of a tower of total measure
EX1
= +oo, and so theProposition
proves the Theorem of the abstract. Also we derive as acorollary
aninteresting example
for thesimple
random walk. Note that the interarrival times of asimple
random walk to theorigin satisfy
thehypotheses
of theProposition
with a =
1 /2.
Therefore the returns of the walk to theorigin
are almostsurely
a bad sequencealong
which totry
to form apointwise ergodic
theorem.
Annales de l ’lnstitut Henri Poincaré - Probabilités et Statistiques
The
key point
of theproof,
much as in Theorem 4 of[LPRW],
is toisolate an
unfortunate,
but almost sure,random
fluctuation with the aid ofa functional law of the iterated
logarithm (LIL).
Animportant
differenceis that in the current
setting
there is no lim sup LIL for Tn =]L~=i Xm
because of the infinite mean. Instead there is a lim inf
LIL,
and inparticular
there is the
following Corollary
to the main result of Wichura[W].
Weneed some notation. Define random functions on
[0, 1] by
Here, [ . ] is
thegreatest integer function,
Ln = e Vlog
n, LLn =log (Ln),
and
Ka
is anormalizing
constant.For
large integers M,
setThe
important
features off
are that for all k > 0and for 0 k M the functions of 0 on the
right
side of( 1 )
areessentially orthogonal
on0 ~ ~
1.LEMMA. - With
probability 1, for
every M there is a(random)
sequenceof integers
nk(w)
= nk such thatThe convergence is to be understood in the sense of convergence in
distribution, viewing Fn (., c~ )
andf ( . )
as random variables defined onthe
probability
space[0, 1].
The reader who refers to
[W]
will have topatiently
unwind definitions to find this Lemma. Aaronson and Denker[AD]
havegeneralized
Whichura’ sresults,
and most readers will find their paper easier to refer to.Proof of Proposition. -
We will invokeBourgain’s Entropy
Criterion[B].
To this
end,
it isenough
toverify
that for almost all W thefollowing
holds:For every
integer
M there are a subset of theintegers
ofcardinality
Mand g of l2 (Z)
norm 1 so that for all n,n’
E .MVol. 33, n° 4-1997.
494 M. T. LACEY
By transference,
the same assertion holds with Z and the shiftreplaced by
any
aperiodic dynamical system.
This will violate theL2-entropy
criterionand so prove the
proposition.
Fix a
large
M. Thegood
o/s are those whichsatisfy
the conclusion of the Lemma. To defineA4,
first select n for which theapproximation
in(2)
is verygood. Specifically,
choose n so thatfor all
bounded, Lipschitz § :
R(see [D,
p.310]).
Takeand
define g by
where
/3n
=Ka
is thenormalizing
constant in thedefinition of
Fn (t).
This allows us toexploit
the functional LIL.We can now
verify (3)
as follows. For m ~nM-k
andnM-k’
in
A4,
These last two sums can be
expressed
asintegrals
ofFn (t).
In(4)
we usefor ø (x)
a differentiable extension e(x)
of(the
real orimaginary part of) (t)
which is boundedby
1 and has derivativebounded
by /3n
B.Then, using (4),
thepreceding expression
is estimatedby
Annales de l’Institut Henri Poincaré - Probabilités et Statistiques
Recalling ( 1 ),
we see that this isessentially equal
to2, finishing
theproof
of
Proposition.
DI am
grateful
to MateWierdl,
and Karl Petersen.They provided
theinspiration
for this paper.REFERENCES
[AD] J. AARONSON and M. DENKER, On the FLIL for certain 03C8-mixing processes and infinite measure-preserving transformations, (English. French summary),
C. R. Acad. Sci. Paris, Série I, Math., Vol. 313, 1991, pp. 471-475.
[BL] A. BELLOW and V. LOSERT, The weighted pointwise ergodic theorem and the individual ergodic theorem along subsequences, Trans. Amer. Math. Soc., Vol. 288, 1985, pp. 307-345.
[B] J. BOURGAIN, Almost sure convergence and bounded entropy, Israel J. Math., Vol. 63, 1988, pp. 79-97.
[BFKO] J BOURGAIN, H. FURSTENBERG, Y. KATZNELSON and D. ORNSTEIN, Return times of
dynamical systems, Appendix to : Pointwise ergodic theorems for arithmetic sets, by J. Bourgain, Pub. Math. I.H.E.S., Vol. 69, 1989, pp. 5-45.
[D] R. M. DUDLEY, Real Analysis and Probability, Wadsworth & Brooks/Cole, Pacific Grove, Gal., 1989.
[LPRW] M. LACEY, K. PETERSEN, D. RUDOLPH and M. WIERDL, Random ergodic theorems
with universally representative sequences, Ann. Instit. H. Poincaré, Vol. 30, 1994, pp. 353-395.
[W] M. WICHURA, Functional law of the iterated logarithm for the partial sums of i.i.d.
random variables in the domain of attraction of a completely asymmetric stable law, Ann. Probab., Vol. 2, 1974, pp. 1108-1138.
[WW] N. WIENER and A. WINTNER, Harmonic analysis and ergodic theory, Amer. J. Math.,
Vol. 63, 1941, pp. 415-426.
(Manuscript received December 21, 1995;
revised November 20, 1996.)
Vol. 33, n° 4-1997.