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Publié par | profil-zyak-2012 |
Nombre de lectures | 14 |
Langue | English |
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AVervaat-likepathtransformation
forthereflectedBrownianbridge
conditionedonitslocaltimeat
0
PhilippeChassaing
1
&SvanteJanson
2
Summary.
WedescribeaVervaat-likepathtransformationforthereflectedBrownian
bridgeconditionedonitslocaltimeat0:uptorandomshifts,thisprocessequalsthetwo
processesconstructedfromaBrownianbridgeandaBrownianexcursionbyaddingadrift
andthentakingtheexcursionsoverthecurrentminimum.Asaconsequence,thesethree
processeshavethesameoccupationmeasure,whichiseasilyfound.
Thethreeprocessesariseaslimits,inthreedifferentways,ofprofilesassociatedto
hashingwithlinearprobing,or,equivalently,toparkingfunctions.
Keywords.
Brownianbridge,Brownianexcursion,localtime,pathtransformation,
profile,parkingfunctions,hashingwithlinearprobing.
A.M.S.Classification.
60J65(primary),60C05,68P10,68R05(secondary).
Runninghead.
Brownianbridgepathtransformation.
1
InstitutElieCartan,BP239,54506VandoeuvreCedex,France.
2UppsalaUniversity,DepartmentofMathematics,POBox480,75106Uppsala,Sweden
1
•••1Introduction
WeregardtheBrownianbridge
b
(
t
)andthenormalized(positive)Brownianexcursion
e
(
t
)asdefinedonthecircle
R/Z
,or,equivalently,asdefinedonthewholerealline,being
periodicwithperiod1.Wedefine,for
a
≥
0,theoperatorΨ
a
onthesetofbounded
functionsonthelineby
Ψ
a
f
(
t
)=
f
(
t
)
−
at
−
−∞
in
<
f
s
≤
t
(
f
(
s
)
−
as
)
=sup(
f
(
t
)
−
f
(
s
)
−
a
(
t
−
s
))
.
(1.1)
ts≤If
f
hasperiod1,thensohasΨ
a
f
;thuswemayalsoregardΨ
a
asactingonfunctionson
R/Z
.Evidently,Ψ
a
f
isnonnegative.
Inthispaper,weprovethat,forevery
a
≥
0,thethreefollowingprocessescanbe
obtained(inlaw)fromeachotherbyrandomshifts,thatwewilldescribeexplicitly:
X
a
,whichdenotesthereflectingBrownianbridge
|
b
|
conditionedtohavelocaltime
atlevel0equalto
a
;
Y
a
=Ψ
a
b
;
Z
a
=Ψ
a
e
.
Wewillfindconvenienttousethefollowingformulasfor
Y
a
and
Z
a
:
Y
a
(
t
)=
b
(
t
)
−
at
+sup(
as
−
b
(
s
))
,
t
−
1
≤
s
≤
t
Z
a
(
t
)=
e
(
t
)
−
at
+sup(
as
−
e
(
s
))
.
t
−
1
≤
s
≤
t
For
t
∈
[0
,
1],wealsohave
Z
a
(
t
)=
e
(
t
)
−
at
+sup(
as
−
e
(
s
))
,
(1.4)
ts0≤≤consistentlywiththenotationsof[13].
Givenastochasticprocess
X
andapositivenumber
t
,welet
L
t
(
X
)denotethelocal
timeoftheprocess
X
atlevel0,ontheinterval[0
,t
],definedasin[10,p.154]by:
t1L
t
(
X
)=l
ε
i
↓
m
0
1
{−
ε<X
s
<ε
}
ds
;
ε20withthisconvention,e.g.,
b
and
|
b
|
havethesamelocaltimeat0,while,accordingtothe
usualconvention[28,
§
VI.2],thelocaltimeat0of
|
b
|
istwicethelocaltimeat0of
b
.When
possible,weextend
L
(
X
)to
t
∈
(
−∞
,
0),insuchawaythat
L
b
(
X
)
−
L
a
(
X
)isthelocal
timeoftheprocess
X
atlevel0,ontheinterval[
a,b
],foranychoice
−∞
<a<b<
+
∞
.
Thedefinitionaboveof
X
a
isformallynotpreciseenough,sinceitinvolvesconditioning
onaneventofprobability0.However,thereexistson
C
[0
,
1]auniquefamilyofconditional
distributionsof
|
b
|
(or
b
)given
L
1
(
b
)=
a
whichisweaklycontinuousin
a
≥
0[25,Lemma
12],andthiscanbetakenasdefiningthedistributionof
X
a
.Theprocess
X
a
hasbeenan
objectofinterestinanumberofrecentpapersinthedomainofstochasticcalculus:its
2
1()2.)3.1(
distributionisdescribedin[27,Section6]byitsdecompositioninexcursions.Thesequence
oflengthsoftheexcursionsiscomputedin[7],using[24].Thelocaltimeprocessof
X
a
isdescribedthroughanSDEinarecentpaper[25]byPitman,whoinparticularproves
that,uptoasuitablerandomtimechange,thelocaltimeprocessof
X
a
isaBessel(3)
bridgefrom
a
to0[25,Lemma14].(Seealso[5],whereaBrownianbridgeconditionedon
itswholelocaltimeprocessisdecribed.)
While
X
a
appearsasalimitinthestudyofrandomforests[25],
Z
a
appearsasa
limitinthestudyofparkingproblems,orhashing(see[13]),anoldbutstillhottopic
incombinatoricsandanalysisofalgorithms,theselastyears[1,14,17,19,26,31,32].
Thefragmentationprocessofexcursionsof
Z
a
appearsinthestudyofcoalescencemodels
[8,9,13],anemergenttopicinprobabilitytheoryandanoldoneinphysicalchemistry,
astronomyandanumberofotherdomains[4,Section1.4].See[4]forbackgroundandan
extensivebibliography,andalso[3,6,16]amongothers.Asexplainedlater,
Y
a
istightly
relatedto
Z
a
throughapathtransformation,duetoVervaat[33],connecting
e
and
b
.
Remark1.1
For
a
=0,wehave
X
0
la
=
w
e
[25,Lemma12]and,trivially,
Y
0
=
b
−
min
b
and
Z
0
=
e
,andtheidentityuptoshiftofthesereducestotheresultbyVervaat[33].
For
a
positive,thethreeprocesses
X
a
,
Y
a
and
Z
a
donotcoincidewithoutshifting.This
canbeseenbyobservingfirstthata.s.
Y
a
>
0,while
X
a
(0)=
Z
a
(0)=0,andsecondly
that
Z
a
a.s.hasanexcursionbeginningat0,i.e.inf
{
t>
0:
Z
a
(
t
)=0
}
>
0(see[8],
wherethedistributionofthisexcursionlengthisfound),whilethisisfalsefor
X
a
(asa
consequenceof[27,Section6]).Italsofollowsthat
Z
a
isnotinvariantundertimereversal
(while
X
a
and
Y
a
are).
Wementiontwofurtherconstructionsoftheprocessesabove.First,let
B
beastandard
one-dimensionalBrownianmotionstartedat0,anddefine:
τ
t
=inf
{
s
≥
0:
L
s
(
B
)=
t
}
.
Then
X
a
canalsobeseenasthereflectedBrownianmotion
|
B
|
conditionedon
τ
a
=1,see
e.g.[25,thelinesfollowing(11)]or[27,identity(5.a)].
Secondly,define
b
˜(
t
)=
b
(
t
)
−
01
b
(
s
)
ds
.Itiseasilyverifiedthat
b
˜isa
stationary
Gaussianprocess(on
R/Z
oron
R
),forexamplebycalculatingitscovariancefunction
Cov(
b
˜(
s
)
,b
˜(
t
))=1
−
6
|
s
−
t
|
(1
−|
s
−
t
|
)
,
|
s
−
t
|≤
1
.
21Since
b
and
b
˜differonlybya(random)constant,
Y
a
=Ψ
a
(
b
˜)too.Thisimpliesthat
Y
a
is
astationaryprocess.(
X
a
and
Z
a
arenot,againbecausetheyvanishat0.)
Wemaysimilarlydefine
e
˜(
t
)=
e
(
t
)
−
01
e
(
s
)
ds
,andobtain
Z
a
=Ψ
a
(
e
˜),butwedo
notknowanyinterestingconsequencesofthis.
Precisestatementsoftherelationsbetweenthethreeprocesses
X
a
,
Y
a
and
Z
a
are
giveninSection2.Thethreeprocessesariseaslimits,underthreedifferentconditions,
ofprofilesassociatedwithparkingschemes(alsoknownashashingwithlinearprobing).
ThisisdescribedinSections3and4.Theproofsaregivenintheremainingsections.
3
2Mainresults
Inthissectionwegiveprecisedescriptionsoftheshiftsconnectingthethreeprocesses
X
a
,
Y
a
and
Z
a
,inallsixpossibledirections.Let
a
≥
0befixed.
First,assumethattheBrownianbridge
b
isbuiltfrom
e
usingVervaat’spathtrans-
formation[10,11,33]:givenauniformrandomvariable
U
,independentof
e
,
b
(
t
)=
e
(
U
+
t
)
−
e
(
U
)
.
(2.1)
nehTΨ
a
b
(
t
)=Ψ
a
e