A NNALES DE L ’I. H. P., SECTION B
D AVID H OBSON
Asymptotics for an arcsin type result
Annales de l’I. H. P., section B, tome 30, n
o2 (1994), p. 235-243
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Asymptotics for
anArcsin type result
David HOBSON
The Judge Institute of Management Studies, Fitzwilliam House,
32, Trumpington street, Cambridge, CB2 IQY, U.K.
Vol. 30, n° 2, 1994, p. 235-243. Probabilités et Statistiques
ABSTRACT. - Let
Ar
be the amount of time that a Brownian motionspends
above 0 before time t. For fixed t the ratioAr/t
has distributionindependent
of t; viewed as a function of time can becomearbitrarily
small. In this paper we consider the effect of
modifying
the denominator.In
particular, if f is
monotonic then or ooaccording
m _
as
~ Jf (t) (dt/t) diverges or converges.
The
proof
considersAr
at the ends of"long" negative
excursions and involvesshowing
the existence ofinfinitely
many such excursions.Key words : Brownian sample path, Arcsin law, Excursion theory.
RESUME. - Soit
Ar
le tempspasse
par le mouvement brownien au-dessus de zero avant le temps t. Pour tdonne.
le rapportAr/t
a une distribution
independante
de t; et lim Dans cetarticle,
nous nous interessons aux
consequences
d’une modification du deno- minateur. Nous montrons que, sif
est une fonctiondecroissante,
roo _
alors lim inf At/tf(t) = 0 si f(t)(dt/t)=~ et si
La demonstration s’intéresse a
At
a la suite d’excursionsnegatives prolongees
et met en relief l’existence d’une infinite d’excursions.A.M.S. Classification : 60 G 17, 60 J 65.
Annales de l’lnstitut Henri Poincare - Probabilités et Statistiques - 0246-0203
Vol. 30/94/02/$ 4,00/ © Gauthier-Villars
236 D. HOBSON
1. MAIN RESULTS
The
proportion
of time that a Browniansample path spends
above zerobefore a fixed time t is
independent
of t and is characterisedby
the arcsinlaw.
Many
other functionals ofsample paths
inherittime-scaling properties
from Brownian motion. In this paper we consider the
asymptotic
behaviourof these functionals.
Define
Then
Atl t
has the arcsin distribution:We consider
for suitable functions
f. For f the
unitfunction f(t)
--_ 1 we can use(2)
and the
Hewitt-Savage
0-1 Law to concludeWe consider when
(4)
is true for otherfunctions f.
Suppose
thatCt
is anadapted
functional of a Browniansample path
and that
Ct
has theproperties
C 1 0 and
Cr increasing;
C 2
Ct
constant onnegative
Brownianexcursions;
C 3
Ctlt
has distribution Findependent of t,
andWe prove our results in terms of the functional
Ct;
notice thatAt
satisfiesthese
conditions,
as doesJt
whereAnnales de l’lnstitut Henri Poincare - Probabilités et Statistiques
THEOREM 1. -
Suppose f
isdecreasing.
ThenSince we obtain an
integral
test forf
somemonotonicity
condition is essential. Also weonly
need thehypothesis
to hold in aneighbourhood
of
infinity,
since we canchange
the definition off
on some compact interval withoutaltering
either the statements or conclusions of Theorem 1.The
analogous
theorem for small times is as follows:THEOREM 2. -
Suppose
g isincreasing.
ThenA
higher
dimensional version of thisquestion
has beeninvestigated by
Mountford
[3]
andMeyre [2].
Mountford considered theproportion
oftime that
planar
Brownian motionspends
in awedge,
normalisedby
thefunctions
f(t)= (log t) -p. By considering
thewedge
ofangle x
we canspecialise
his result to one dimension:Meyre
considered the d-dimensional case, and the amount of time spent in a closed cone with vertex 0by
a Brownian motion.Again considering
functions of the
form f (t) _ (log t)-P,
he extended the results of Mount- ford and showed inparticular
thatfor p = 2
Both authors derived their results
by finding
anincreasing
unboundedsequence of times at which the Brownian motion was
relatively
far fromVol. 30, n° 2-1994.
238 D. HOBSON
the
origin,
and thenshowing
that it would sometimes take a"long"
timeto leave the relevant
wedge
or cone. In this paper we use excursion arguments which arespecific
to one-dimension to prove a more sensitiveresult. °
The remainder of the paper is structured as follows. In section 2 we use
Borel-Cantelli type arguments to prove
In section 3 we
complete
theproof
of Theorem 1by considering
the valueof
Ct
at the ends of"long"
excursions from zero. In Section 4 we deduce Theorem 2by considering
the mapBt t B1/t.
I am
pleased
toacknowledge
the assistance with the excursion argumentsprovided by
Professor ChrisRogers.
2. PROOF OF THEOREM 1
(i )
For fixed r >
1,
KThen
using
the factthat f is decreasing
we haveand then
by
the First Borel-Cantelli Lemmaand
Ct/tf (t)
>K/r eventually,
almostsurely.
3. PROOF OF THEOREM 1
(ii)
In order to prove Theorem 1
(ii)
we consider the excursion process ofBI
from 0. Theprinciple underlying
theproof
is that low values ofCt/tf (t)
will occur near the ends of
long negative
excursions. We define"long"
Annales de l’Institut Henri Poincaré - Probabilités et Statistiques
excursions in an
f dependent
way such that is less than E nearthe end of such
excursions;
the result follows if we can provethat,
foreach E, there are an infinite number of
long excursions.
A feature of the
proof
is that it is not necessary to consider combinations of two or morelarge negative
excursionsfollowing
soon after one another.By hypothesis f
isdecreasing
and without loss ofgenerality
we mayassume that
f (t) _ 1
andf (t) ,~ 0;
otherwisereplace f by
First we establish some suitable notation: let
Lt
be the local time(of B)
at 0
by time t,
and let so that yi is a subordinator.Classify
an excursion at local time I as along
excursion if itslifetime ç
satisfies
Classify
it as along-early
excursion if also l2. If i = yl _ is the time at which along-early
excursionbegins then,
It remains to show that there is an
increasing
unbounded sequence ofnegative long-early excursions;
Theorem 1(ii )
then followsimmediately.
Define
The
integrand
in(14)
follows from the fact that the rate of excursions whose lifetimeexceeds ç
is(2/~~) 1 ~2 (see
forexample [I],
p.129,
but beware normalisations of the local time which introduce extra factors of2).
Note thatsince f (~) _
1For l > 1 let
Nl
be the number ofnegative long-early
excursions between local times 1 and I.(We
startcounting
at local time 1 to avoid thepotential complication
of an infinite number oflong
excursionsoccuring
Vol. 30, n° 2-1994.
240 D. HOBSON
immediately
at time0.)
Ourproof
thatis
completed
in two stages.PROPOSITION 3 . 1 : 1
Proof. -
Letand define The rate of
negative long-early
excursions at local time u is amultiple 1 2I{03B3u~u2}
of the rate oflong
excursionsgiven
in(14).
Thus V is the compensator for N and M is a
martingale.
We need toprove that
N~
= oo almostsurely
if andonly
ifV~
= oo almostsurely.
M is a
martingale
with boundedjumps.
Mstopped
when it first falls to - k is amartingale
boundedbelow;
thus it converges almostsurely
toa finite limit. If
N~
= oo then thestopped martingale
canonly
convergeby reaching - k;
since k isarbitrary
it follows that lim infM, = -
thusVoo=oo.
Conversely
ifV~
= oo then a similar argumentapplied
to Mstopped
on first
rising
above k shows that lim supM,
= oo almostsurely;
henceNoo=oo.
DPROPOSITION 3.2: 1
Proof -
IfV ~
= oo thencertainly
which can be shown
by
a few lines of calculus to beequivalent
to theright
hand side of(16).
Conversely
letK~=1~~2~ and
We prove that ourintegral
condition
on f is equivalent
to ~,li
oo and hence that(V~
= oo, a.s.)
asrequired.
Note that where
L and S are the local time and maximum processes of a Brownian motion
Annales de l’Institut Henri Poincare - Probabilités et Statistiques
and N is a standard normal random variable. In
particular
i
r
define c = E
(K~)
= !P{ y~ ~ }, independent
of ~;then
= - c~ (~)
~M.~
Ji
and
for some constant k. This estimate can be used as follows:
for some constant
D,
this last linefollowing
from(15).
Since oo wehave
For any
large
constant A we can choose ssufficiently large
so thatwhence
using Tchebyshev
Thus
(V~
= oo, a.s.)
asrequired.
D4. ASYMPTOTIC RESULTS FOR SMALL TIMES
In this section we deduce Theorem 2.
Suppose g : (0, 1] ] ~ f~ +
is increas-ing.
Vol. 30, n° 2-1994.
242 D. HOBSON
PROPOSITION 4. 1 : 1
Proof. - By considering
down thegeometric
sequence r-n andmirroring
theproof of §
2 it ispossible
to obtainUsing g (s) increasing
we haveand
Cslsg (s)
>K/r eventually.
DPROPOSITION 4.2: 1
Proof. -
For the same reasons as in§ 3
we may assume thatg (s) 1 and g (o + ) = o. Define , f ’ : [ 1, oo)-~[0, 1] ] by f (t ) = g (s)
where Thenf is decreasing.
AlsoBy
the resultsof §3
there are an infinite number ofnegative
excursions
(to, ti)
oflifetime §
= t 1 - to whichsatisfy both f (ç)
>to/E
and~ > to.
This second condition is not restrictive forlarge
timessince f (t) ~,
0.If
Bt
is a Brownian motion then so is Hence if(to, tl)
is aBrownian excursion for B then
(si, so)
is aW-excursion,
where si =i = o,
1. Then ifCs
is defined relative to the Brownian motionW~
and if(to, tl)
is along
excursion forWS/s
But
CS 1 _ s 1
andsince ~ >
to andf
isdecreasing
Annales de l’Institut Henri Poincare - Probabilités et Statistiques
REFERENCES
[1] N. IKEDA and S. WATANABE, Stochastic Differential Equations and Diffusion Processes, North Holland-Kodanska, Amsterdam and Tokyo, 1981.
[2] T. MEYRE, Étude asymptotique du temps passé par le mouvement brownien dans un
cône, Ann. Inst. Henri Poincaré, Vol. 27, 1991, pp. 107-124.
[3] T. S. MOUNTFORD, Limiting Behaviour of the Occupation of Wedges by Complex
Brownian Motion, Prob. Th. Rel. Fields, Vol. 84, 1990, pp. 55-65.
[4] L. C. G. ROGERS, A Guided Tour Through Excursions, Bull. London Math. Soc., Vol. 21, 1989, pp. 305-341.
(Manuscript received June 18, 1992;
revised October 1 , 1992.)
Vol. 30, n° 2-1994.