D AVID G. H OBSON
Marked excursions and random trees
Séminaire de probabilités (Strasbourg), tome 34 (2000), p. 289-301
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Article numérisé dans le cadre du programme Numérisation de documents anciens mathématiques
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David G. Hobson
Department
of MathematicalSciences, University
ofBath,
Claverton
Down, Bath,
BA2 7AY. UK.1 Introduction
This article is devoted to the
study
of theproperties
of a marked Brownianexcursion,
and an
embedding
of abranching
tree in an excursion with marks. Theembedding depends
upon theheights
of the excursion at the various marktimes,
and theheights
of minima between consecutive marks. The
resulting
tree is a criticalbinary
treewith an
independent branching
structure. The construction alsogives
rise to anatural connection between a Brownian excursion with at least one
mark,
and afamily
of Brownian excursions each withexactly
one mark.The
relationship
between Brownian excursions and trees has been muchexplored
in the
literature,
a selection of which we note here. Neveu and Pitman[9, 10]
(see
also Le Gall[5])
considered excursions ofheight
at leasth,
and embedded a tree in the excursion based on the locations of h-maxima andh-minima,
which are excursiondependent
local-extremes(see [9, 10]
fordefinitions.)
LeGall[6]
hasdescribed one fruitful
application
of therelationship
between excursions and trees to the construction of super-processes.Aldous
[1, 2, 3]
based a tree on the excursion value atarbitrary
times chosenindependently
of the excursion structure. His tree, the Brownian continuum random tree contains an infinite number of ’leaves’. Le Gall[7]
considers a tree with a finitenumber of leaves which
correspond
to times chosenuniformly
over the lifetime of aBrownian excursion. This article has much in common with this last paper.
Le Gall chooses an excursion
according
to Ito measure,re-weighted by
thelength
7 of the
excursion,
andimagines putting
ppoints uniformly,
andindependently,
inthe interval
[0,
He then defines a construction of a tree based upon theexcursion,
and inparticular
the excursion values at thesetime-points.
Here weimagine
aBrownian motion and an
independent
Poisson processmarking
the time axis. We consider the first Brownian excursion to contain amark,
orequivalently
we choosean excursion
according
to the Ito measure of marked excursions. This first marked excursion contains a random number ofmarks,
butby
theproperties
of the Poissonprocess, each mark is
uniformly
distributed over the lifetime of the excursion. Nowwe have an excursion with a
(random)
number of identifiedpoints
and we can definean embedded tree in the manner of Le Gall
[7].
Weinvestigate
theproperties
of theresultant tree: since the excursion and the marks have been chosen in a
canonically simple fashion,
theresulting
tree is alsoparticularly simple.
We extend this idea to construct a second tree in which each node of the tree
corresponds
to a mark in theoriginal excursion,
and in the final section use thisconstruction to
explain
an observation on the Arcsin law.In this article we consider marked excursions. A related
problem involving
nor-malised excursions
(ie
excursions of unitlength)
has been consideredby
Pitman[12].
Pitman derives the
joint
distribution of the values of a normalised Brownian excur-sion at times 0 ~ ~ ~
U(n~
1 and the minima of the process over subintervals(~U~i), U(i+1)~)1in-1~
. HereU(1), ...
are the order statistics of nindependent
standard uniform random variables. The choice in this paper of excur-sions which contain a mark introduces a size bias which is
exactly
theright
factorto
guarantee
theindependent branching
structure of the embedded tree.It is a
pleasure
to thank Jean-Francois Le Gall for discussions andcorrespondence
on this
subject,
and an anonymous referee whose detailedreading
of an earlierversion of this
manuscript
ensured that this version is much clearer.2 Preliminaries
onTrees
2.1 Trees
A tree consists of a finite
family
of elements ordered intogenerations.
The zerothgeneration
contains asingle parent
individual who has a random number ofoffspring.
These
offspring
form the members of the firstgeneration. Subsequently
each member of thekth generation
has a random number ofoffspring
who formpart
of thegeneration.
Formally, following
Neveu[8],
define a tree asfollows;
T is a tree if T is a finitesubset of U :=
U=o,
where~J°
:={0},
such that.
~ for k >
1,
if u = ul ... u~ E T then ul ... E T;. for k >
1,
if u = ul ... u~ E T with uk = n then u = ul ... uk-lm E T for1 m ?~. ’
Let T be the set of trees, and if u = ul ... uk let
~u)
= k.2.2
Marked
treesA marked tree is of the form
where T and
Lu
E ‘du E T. The markLu
should beinterpreted
as thebranch
length
or lifetime of the individual associated with element u.Let T
be the space of marked trees.Note the unfortunate dual use of the word marked. In an excursion a mark refers
simply
to an identified time. In a tree a mark is apiece
of additional information associated with an element.Hopefully
no confusion will arise.2.3 Binary
trees .In a
binary
tree the number ofoffspring
isalways
either zero or two. LetTb
be theset of
binary
trees. Introduce a measure onTb by setting
~c(T)
=where 11711
is thecardinality
of T. The measure v models abranching
process with abinary branching
distribution where each individual has zero or twooffspring
withprobability 2 .
If p := E T : ~l~ T} (~
then p is the number of elements of the tree with no descendents =2p - 1.
Such elements are termed ’leaves’ ofthe
tree.
’
Let
Tb
be the space of markedbinary
trees. For apositive
define a measure ~aon
~b by setting
=
dLu)
:_~~T)
This measure
corresponds
to a continuous timebranching
process withoffspring
distribution the uniform measure on
{o, 2},
andexponential,
rate a, lifetimes. Inparticular,
for u E T, the law of the subtree rooted at u is the same as the law ofthe whole tree..
Figure
1: Arepresentation
of a markedbinary
tree. Vertical distancescorrespond
to the branch
lengths.
Note that the horizontal scale andspacings
are notpart
ofthe definition of the tree.
2.4
Binary
treesand excursions
Define the set E of excursions to be the
family
of functions e : :l~+.
e u Awith an associated lifetime 7 =
a(e)
E14
such thate(0)
=0, limstu e(s)
=0,
e iscontinuous on
[0, ~)
andpositive
on(0, ~),
ande(s) = ~,
Vs > ~. The element A isa
graveyard
state. We willloosely
define an excursionby describing
it’s lifetime uand a continuous function e :
[0, o-)
~R+
with theappropriate properties.
In thesequel
we will also use theconcept
of an excursion started from h >0,
which is as aboveexcept
thate(0)
= h. We will alsospecify time-points
0 si ... sp Qduring
the lifetime of an excursion. Thesepoints
will be identified with leaves on an associated tree. LetEp
be the space ofexcursions,
with pspecified time-points,
and let
E - Ei.
Given an excursion e, for a finite
integer
p, fix 0 si ... sp a. Then in each interval[sr, (r =1, ... p -1),
there exists a time tT such that the infimum of e over the interval is attained at tr. Assumethat tr
isunique
and in the open interval(sr; sT+1 ),
and further that the valuese(tj) are
distinct. When we consider Brownian excursions theseassumptions
will besatisfied,
almostsurely.
Figure
2: Aplot
of atypical
excursion e up to its lifetime 7, with identifiedpoints
si ... s6 cr. The time t at which the infimum of e over
ss]
is attained is alsoshown,
as are t- andt+.
Suppose, inductively,
that we aregiven
a label u E T, an associated excursion eu, and an ordered set of times 0 ...Initially
we take u -0,
e~ == e, and ... ,
sp~u)) _ (sl, ... , sp).
Thene if
p(u) = 1,
set u to be aleaf,
so that u1~
T and u2~
T. LetLu
=eu(si )
andeu -
eu. Note thate~,
EE.
e if
p(u)
>1,
let tu be thetime-point
between the first mark(at si)
and the last mark(at
at which the excursion eu attains its minimumvalue,
so thateu(tu)
=eu(t).
Associate with the label u thelength Lu
-Moreover,
setu1,
~2 E T. We wish todecompose
eu into threeexcursions;
anexcursion
eu
withexactly
one labelledpoint,
and two other excursions eul, eu2,each with at least one labelled
point.
Define the times tu- ~ supssnl{eu(s) =eu(tu)} and tu+
=infs>sup(u) {eu(s)
=eu(tu)}.
The threecomponents
of thedecomposition
are then as follows:eul(s)
:=eu(t" +s) -eu(t")
is an excursionwith lifetime tu -
eu2(s)
:=eu(tU
+s) -
anexcursion
with lifetime(t+ - t");
andeu(s)
which has lifetime(t+ -
and isgiven by eu(s)
:=eu(s)
for andeu(s)
= +s),
for s > t"For the label u E T this construction defines a mark
Lu
and associated excursioneu
EE. Moreover,
whenp(u)
> 1 the constructionproduces
two sub-excursions labelled u1 and~2,
with marks(s"1 . s"1 ) - (su -
...su -
and(s’~2
... ,su2 ) -
(S~+i - tu,
... ,, sp(~~ - respectively, where j
=sup{k : : sk
Figure
3: A A-markedexcursion,
andsuperimposed
the associated tree with sixleaves, corresponding
to the six marks.Since p is finite this construction must
terminate,
toproduce
a marked tree(T, (Lu,
u ET)),
and afamily
of excursions(eu,
u ET).
Note that each member of thisfamily
of excursions hasexactly
one identifiedpoint
whichcorresponds
eitherto one of the
original marks,
or to one of thesplit
times tr.The first aim of this article is to describe the law of the marked tree, and the associated
excursions,
when theoriginal
excursion is chosen to be a marked Brownian excursion.3 Ito excursions and marked trees
Let B be a Brownian motion with local time
process
at zero.Then,
as Itoobserved,
B can be
decomposed
into excursions away from zero, indexedby
l. These excursions form a Poisson process, on the space of excursions(as
definedabove,
but also withthe choice of
sign),
withintensity n(de). By saying
that ’e is a Brownian excursion’we mean that e has been chosen
according
to n.Suppose
further that time is markedby
anindependent
Poisson process with constantintensity
A. For an excursion e, with duration cr =r(e),
theprobability
that there are k marks is
By properties
of the Poisson process theintensity
of Brownian excursions e with k marks at 0 si ... cr isdsi
...,)
=n(de) dsl ds k
,
a T
We will say that ’e is a A-marked excursion’ or
just
’e is a marked excursion’ if e is chosenaccording
to n and the time domain of e contains at least one mark of the Poisson process.For Brownian motion
B,
with local time process A and firsthitting
timesH,
and for
Ta
the time of the first mark of theindependent
Poisson process, we have>
z)
=P(Hz Ta)
= E(~Hz03BBe-03BBtdt)
= E(e-03BBHz) =
e-z203BB. (1)
Here the first
equality
is based onLevy’s
Theoremidentifying
the law of the local time of Brownian motion with the law of the maximum. It follows that the rate of marked excursions is and that theprobability density
of an excursion e withk marks at 0 s1 ... 03C3k 03C3, conditional on the excursion
having
amark,
is03BB,k(de,ds1,.., dsk)
= n(de)03BBke-03BB03C3 203BBds1...dsk
Let 03BB = 03A3k>1
ñ03BB,k be the probability density
of an excursion with associated Poissonmarks,
conditioned to have at least one mark.Theorem 1 Let a =
2B/2A.
Underna
the distributiono f T(e)
is . Moreovereach
of
the associated excursions is a a-marked excursion conditioned to haveexactly
one
mark,
and the excursions associated withdifferent
individuals in the tree areindependent.
In the
proof
of this theorem we need akey
lemma on excursions with asingle
mark.
Lemma 2 A 03BB-marked excursion conditioned to have
exactly
one mark has thef ollowing
structure; theheight
Zof
the mark has anexponential distribution,
ratea, the
post-mark
process is anindependent
Brownianmotion,
started at Z and conditioned to hit zerobefore being marked,
and thepre-mark
process is a time reversalof
afurther independent
Brownianmotion, again
started at Z andagain
conditioned to hit zerobefore being
marked.Proof of Lemma 2 We have that
I > z)
= >z)
=P(Hz Ta)
=(recall (1))
so that theheight
of the first mark in a Brownian motion has an ex-ponential distribution,
rate2a.
Further theprobability
started from z ofhitting
zero unmarked is
e-x 2~’. Hence,
theheight
of the mark in an excursion conditioned to haveexactly
one mark hasdensity proportional
to( 2.1e x 2a)(e-x 2a) -
so that it has an
exponential distribution,
rate a =2~/2A.
It also follows that theprobability
that a A-marked excursion hasexactly
one mark is1/2.
The other statements follow from the
strong
Markovproperty
and the invariance of the excursion measure under time reversal(see Rogers
and Williams[13, VI.49]).
o
Given an excursion e, started from h >
0,
definee(s) -
Thenby Levy’s Theorem,
if e is a Brownian excursion run until it first hits0,
then((e - e)(s), s
>0)
is a reflected Brownian motion started at 0 and run until the local time at 0 first reaches h.Further,
if e is a Brownian motion conditioned to have nomarks,
then the excursions of(e - e)
from 0 are Brownian excursions conditioned to have no marks.Proof of Theorem 1
Let e be a A-marked Brownian excursion with lifetime u. Let
Tl
be the time ofthe first
mark,
andlet ç == e(Tl)
be theheight
of the first mark.Then ç
has anexponential
distribution with rate2a
and ifeT(s)
=e(Ti
+s)
then the process(eT - eT)
is areflecting
Brownianmotion, independent
of~,
run until the local time at 0 reaches~.
For s r 2014Ti
defineY(s)
:=(eT - s).
The process Y isa
reflecting
Brownian motion run until it’s local time at zero first reaches~,
but wecan think of it as the first part of a
reflecting
Brownian motion run for alltime,
andalso labelled Y. We are interested in the last marked excursion from 0
(if any)
ofthe process e -
e,
thiscorresponds
to the first marked excursion of the time reversed process Y(if
that excursion occurs before the local time at zero reaches~.)
The first A-marked excursion of Y occurs when the local time at 0 reaches r~ where r~ has an
exponential
distribution with rate(again
recall(1)).
Theprobability
that the excursion e has
exactly
one mark isprecisely
theprobability that ç
r~,namely one-half,
and moreover the law of r~ isexponential
rate a =Consider the case
where ~
Conditionalon ~
yy the excursion e containsexactly
one mark at aheight ~
which has anexponential
rate adistribution,
andwe can
apply
thedescription
in Lemma 2.Consequently,
withprobability 1/2,
themarked tree consists of
just
the parentindividual,
who has lifetime~.
Notethat,
conditional
on ~
has anexponential,
rate a distribution.Now consider the case
where q ~.
The process Y contains excursions whichare
unmarked,
followedby
a first marked excursion at local time r~, whichbegins
attime
tY
and ends attt.
Now consider these times in terms of theoriginal
excursione. Let t
:_ ~ - tY
andt+
= u - and let t- := =e(t)~.
Then t, t_,t+
Figure
4: A Brownian excursion e, with first mark atTi
and the process e alsoplotted..
have the
meanings they
weregiven
in Section 2 and the excursion e is divided into threeexcursions,
el, e2,e~ given by el (s)
:=e(t-
+s) - e(t_)
for 0 s t -t_,
e2(s)
:=e(t
+s) - e(t)
for 0 st+ - t
ande~(s)
=e(s)
for st-,
ande~(s)
=e(t+ -
t- +s)
for s > t-.By
construction the time reversal of e2 isa marked excursion of
Y, and, by
invariance under time-reversal of nx, so is e2.Moreover, again by
the invariance under time-reversal of andby
thestrong
Markovproperty,
so is el.Finally, by
Lemma2, 60
isprecisely
a Brownian excursion withexactly
one mark.Recall that
~) = 1/2
so that theprobability
that the excursion containsmore than one individual is one half. Then the marked tree has a
parent
individual(with
lifetime conditional on 7y~,
r~ has anexponential distribution,
ratea)
who has
exactly
twooffspring.
Theseoffspring correspond
to the marked excursions el and e2, which areindependent
of eachother,
and of the excursion60
associatedwith the
parent.
The theorem follows
by
induction. DRemark 3 It follows from the theorem that if we extend the notion of a mark or
label on an element of a tree from a lifetime to an excursion with
exactly
one markor identified time then we have a
correspondence
e H(T, (eu,
u ET))
where e is aÀ-marked Brownian
excursion,
T a criticalbinary
tree, andeu
afamily
of Brownianexcursions conditioned to have
exactly
one mark.4 Equating marks with leaves
Our
goal
in this section is to embed a different tree, p, in a marked Brownian excursion. This new tree has one node(rather
than oneleaf)
for each mark inthe excursion. The motivation for consideration of this new tree is a
Ray-Knight interpretation
of excursions and local times at different levels. Anapplication
isgiven
in the next section.Suppose, inductively,
that we aregiven
an individual labelled u E p, an associ- ated excursion eu , and an ordered set of times 0 ...s~(,~} Initially
we take u =
0,
e, and(s~, ... , sp~,~))
_(sl, ... , sp).
Let{e~,(si ), ... ,
be minimised at h = for some i. Associate with the label u the lifetime
Lu
= h. Ifp(u)
= 1 then this individual has nooffspring.
Otherwise there is at leastone excursion above the
height h
which ismarked;
label the d =d(u)
such marked excursionssequentially u1, u2,
... , ud. These excursionscorrespond
to direct de-scendents of u in the tree p.
For j
=1, ... ,
d let be the start of thejth
markedexcursion eu; above
h,
and define new mark timess"~
asappropriate.
Weare now in a
position
torepeat
the construction for these sub-excursions. Since the number of marks p is finite this construction mustterminate,
toproduce
a markedtree
( p, (Lu,
u Ep) )
Theorem 4
Under fix
the distributionof p(e)
is thatof
a critical Galton- Watson process withgeometric offspring
distribution. Inparticular
the measureof
a tree p isv( p)
- . The marked tree has law=
dLu) 2 ~1+d~’~»(1
+uEp
=
v(p) II (1
+uEp
where
d(u)
is the numberof offspring of
the individual labelled u.We prove Theorem 4
by defining
asurjection
from~~
tot.
Given a markedbinary
tree(with
markscorresponding
to individuallifetimes)
associate with eachleaf u = Era total
lapsed time lu
=(the
sum of its own lifetimeplus
the lifetimes of itsancestors).
Let u be the label of the leaf with lowest
lapsed
time. Let thislapsed time lu
be the lifetime of theparent 0
of the marked treep.
Now consider the number of descendents of theparent
individual in thebinary
tree T(excluding
the individualcorresponding
to the leafu),
who are alive at the timelu,
seeFigure
5. Each ofthese individuals is the root of a marked
binary
tree(we
consideronly
thatpart
ofthe sub-tree above
lu),
and to each of these individuals we can associate anoffspring
of the
parent
in p. In this way we can buildinductively
a marked treep
in whicheach
node, including
theleaves, corresponds
to a leaf in T.Proof of Theorem 4
Most of Theorem
4,
and inparticular
theindependent branching
structure, follows from Theorem1,
and inparticular
the fact that the marks have anexponential
Figure
5:Constructing
thegeneral
tree from abinary
tree. In the new tree theparent
has fouroffspring,
the last of whom has oneoffspring. Again
the horizontal scale isunimportant, although
it has been inherited from a Brownian excursion.Note that each node in the new tree
corresponds
to a leaf in the old tree.distribution,
and from themapping f
Hp.
Theremaining part
is toidentify
thejoint
law of the lifetime andoffspring
distribution.Number
of offspring.
Each event in thebinary
tree is withequal probability
either a
split
or a death. The number ofoffspring
of theparent
in p isexactly
thenumber of
splits
before the first death in T(working upwards through
thetree)
andhas a
Geometric, parameter 1/2,
distribution.Each individual alive at this first death is the root of a future tree,
by
theexponential
lifetimeproperty
inf,
each of these trees isindependent
and has thesame
probabilistic
structure as the whole tree.The law
of
thelifetime,
conditioned on the numberof offspring.
Conditionalon the
parent 0 having k offspring,
the lifetimeof 0
is the sum ofindependent exponentials Ta
+T2
+ ... +T(k+1~«.
HereTa,
rate a, is the time until the first event in thebinary
tree, rate2a,
is thesubsequent
time until the secondevent,
(there
nowbeing
two individuals in thebinary tree),
and so on.By
well known facts on the Yule process, orinductively
on the number of off-spring,
the lifetime of theparent,
conditioned on koffspring,
hasdensity fk(t)
=(k
+a
5 Trees and the Arcsin Law
Let
Bt
be a Brownian motion and let~
=(lit) f~
be theproportion
oftime that Brownian motion has
spent positive by
time t. Thenby
Brownianscaling Vt g V,
a random variableindependent
of t which has the Arcsin distribution:P(V ~ v)
=du 03C0u(1-u); 0 ~ v ~ 1.The
original
motivation of thisstudy
was toexplain
and understand the obser- vationthat,
for allintegers k
>0,
lE(Vk)
=2-2k ( ) = P(random
walk oflength
2k isalways non-negative).
Since V is a distribution on
[0,1]
and iscompletely
determinedby
its moments, anexplanation
of this observation can be viewed as an alternativeproof (though hardly
the most
direct)
of the Arcsin Law.The final
equivalence
that we need relates a tree p withm ~
1 individuals toan excursion of a
simple
random walk S with 2msteps.
Given a tree p, definea map
f :
:{ 1, 2, ... , , 2m -1 }
H{u :
: u Ep}
as follows. Letf (1 )
=~.
Given1 (i)
= u = ul ... ukchoose,
ifpossible,
the first child v of u which has notalready
been
visited,
and letf (i
+1)
= v, otherwise letf (i
+1)
=Finally
letSo
=0, ~
=+
1 and~
= A.Standard combinatorial
properties give
that if p is a criticalbranching
process withgeometric parameter 2 offspring distribution,
then theresulting
random walk is an excursion of asimple symmetric
random walk. Thisconstruction,
called thecontour process or
exploration
process, is due to Harris[4],
see also Le Gall[5].
Proposition
5=
P(random
walk oflength
2k isalways non-negative)
Proof.
The
proof
is based upon the observation that thekth
moment of V is theprobability
that for a Brownian
path
with kmarks,
the value of the Brownian motion ispositive
at each of the mark-times. We combine this remark with Theorem 4 and the
bijection
between critical Galton-Watson
branching
processes and excursions of random walks to deduce our result.Let
Tk+i
be the time of the(k+1)th
mark. Consider Brownian motion on[0, Tk+i]
(with exactly
kmarks)
and Conditional onTk+l,
the timesTi
...Tk
are(the
order statisticsof) k
uniform random variables on[0,Tk+1].
ThusE(Vk) ~ E(VkTk+1) + Tk+10...Tk+10I{Bs1>0}
... >0}ds1 Tk+1
...=
P(BTi
Now consider the whole
path
of B. Use Theorem 4 toidentify
thejth
markedexcursion of
B, (with
m~marks),
with ajth
realisation of abranching
tree(with
m~individuals)
and apositive
ornegative
labelaccording
as the Brownian excursion ispositive
ornegative.
Thejth
realisation of thebranching
tree is in one-to-onecorrespondence
with an excursion of asimple symmetric
random walk(with 2~n~
steps).
We use the label of the tree to decide if this is apositive
ornegative
excursionof the random walk. Now
glueing
these excursionstogether gives
us asimple
randomwalk
(Sn,
n >0).
Thepositivity
of ...BTk
isequivalent
to the fact that(Sn
>0)
for every n 2k. 0
For other consequences of the
relationship
between Brownian motionsampled uniformly
at randomtimes,
andsimple
randomwalks,
see Pitman[11, Corollary 3~.
References
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The continuum random tree.I.,
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