• Aucun résultat trouvé

Self-similar fragmentations derived from the stable tree I: splitting at heights

N/A
N/A
Protected

Academic year: 2021

Partager "Self-similar fragmentations derived from the stable tree I: splitting at heights"

Copied!
31
0
0

Texte intégral

(1)

HAL Id: hal-00001550

https://hal.archives-ouvertes.fr/hal-00001550

Submitted on 10 May 2004

HAL is a multi-disciplinary open access archive for the deposit and dissemination of sci- entific research documents, whether they are pub- lished or not. The documents may come from teaching and research institutions in France or abroad, or from public or private research centers.

L’archive ouverte pluridisciplinaire HAL, est destinée au dépôt et à la diffusion de documents scientifiques de niveau recherche, publiés ou non, émanant des établissements d’enseignement et de recherche français ou étrangers, des laboratoires publics ou privés.

I: splitting at heights

Grégory Miermont

To cite this version:

Grégory Miermont. Self-similar fragmentations derived from the stable tree I: splitting at heights.

Probability Theory and Related Fields, Springer Verlag, 2003, 127, pp.423-454. �10.1007/s00440-003- 0295-x�. �hal-00001550�

(2)

ccsd-00001550, version 1 - 10 May 2004

tree I : splitting at heights

Grégory Miermont

DMA , Éole Normale Supérieure,

and LPMA , Université Paris VI.

45, rue d'Ulm,

75230 Paris Cedex 05

Résumé

Thebasiobjetweonsiderisaertainmodelofontinuumrandomtree,alled

thestabletree.Weonstruta fragmentation proess (F(t), t≥0) outofthis tree

byremovingthevertiesloatedunderheightt.Thankstoaself-similarityproperty of the stable tree, we show that the fragmentation proess is also self-similar. The

semigroupand other features ofthe fragmentation aregiven expliitly. Asymptoti

resultsaregiven,aswellasaoupleofrelatedresultsonontinuous-state branhing

proesses.

Key Words. Self-similar fragmentation, stable tree, stable proesses, ontinuous-state

branhing proess.

A.M.S. Classiation. 60J25, 60G52, 60J80.

ResearhsupportedinpartbyNSF GrantDMS-0071448

(3)

1 Introdution

Thereentadvanesinthestudyofoaleseneandfragmentationproessespointedat

thekeyroleplayedbytreestruturesinthistopi,bothatthedisreteandontinuouslevel

[15,3,4℄.Our goalhereis topushfurther the investigation,begunin[3,9℄,of aategory

offragmentationsobtained by utting aertain lass aontinuum randomtree. The tree

that was fragmented in the latter artiles is the Brownian Continuum Random Tree of

Aldous,andthe fragmentationisrelatedtotheso-alledstandardadditiveoalesent.The

family of trees we onsider is a natural but tehnially involved Lévy generalization of

the Brownian tree. It has been introdued in Duquesne and Le Gall [14℄, and impliitly

onsidered in the previous work of Kersting[18℄. Some of these trees, as their Brownian

ompanion,enjoy ertainself-similarproperties. Inthe present work the ruialproperty

is that when removing the verties of the stable tree loated under a xed height (or

distane to the root), the remaining objet is a forest of smaller trees that have the

same law as the originalone up to resaling. This is formalizedin Lemma 3 below. This

way of logging the stable tree indues a fragmentation proess whih by the property

explainedaboveturnsout tobeaself-similarfragmentation,the theoryof suhproesses

being extensively studied by Bertoin [8, 9, 10℄. The goal of this paper is to desribe the

harateristisandgivesomepropertiesofthisfragmentationproess.Wewillhavetouse

stohastiproessesandombinatorialapproahesinthesametime;inpartiular,wewill

enounter σ-nite generalizations of the (α, θ)-partitions of [26℄, whih are distributions on the set of partitions of N = {1,2, . . .}, as well as we will need the onstrution of

the stable tree out of Lévy proesses and its onnetion to ontinuous-state branhing

proesses(CSBP) explainedin [14℄.

In a ompanion paper [23℄ we will onsider another way of obtaining a self-similar

fragmentation by another uttingdevie on the stable tree, using the heuristi fat that

whenuttingatrandomonehub inthe the stabletree,the trunk andbranhes thathave

been separated are saled versions of the initial tree. Surprisingly, although this other

devie looks quite dierent from the rst (no mass is lost when utting a hub, whereas

there is a loss of mass when we throw everything that is loated under the height h), it

turnsoutthatthe onlydierenebetween thesetwofragmentationsisthespeed atwhih

fragments deay.

To state our main results, let us introdue quikly the already mentioned tree stru-

tures and fragmentation proesses, postponingthe detailsto afurther setion.

Let S = {s = (s1, s2, . . .) : s1 ≥ s2 ≥ . . . ≥ 0,P

i≥1si ≤ 1}. A ranked self-similar fragmentation proess (F(t), t ≥0) with index β ∈R is a S-valued Markov proess that

isontinuous inprobability,suh that F(0) = (1,0,0, . . .)and suh that onditionallyon

F(t) = (x1, x2, . . .), F(t+t)has the law of the dereasing arrangement of the sequenes

xiF(i)(xβit), where the F(i) are independent with the same law as F. That is, after time t, the dierent fragments evolve independently with a speed that depends on their size.

Ithas beenshown in[9℄ thatsuh fragmentationsare haraterized by a3-tuple(β, c, ν),

where β is the index, c ≥ 0 is an erosion real onstant saying that the fragments may

melt ontinuously at some rate depending on c, and ν is a σ-nite measure on S that

attributesmass 0to(1,0, . . .) andthat integrates s7→(1−s1). Thismeasure governs the

suddendisloationsinthefragmentationproess,andtheintegrabilityassumptionensures

thatthese disloationsdo not our too quikly,althoughthe fragmentation epohs may

(4)

form a dense subset of R+ as soon as ν(S) = +∞. When β < 0, a positive fration of

the mass an disappear within a nite time, even though there is noloss of mass due to

erosionnortosudden disloations.This phenomenon willberuialinthe fragmentation

F below.

The treeswe are onsideringare ontinuumrandomtrees. Intuitively,they are metri

spaeswithaninnitelyramiedtreestruture,whihanbeonsideredasgenealogial

struturesombinedwithtwomeasures:aσ-nitelengthmeasuresupportedbytheskele-

ton of the tree and a nite mass measuresupported by its leaves, whihare everywhere

densein the tree. These trees an be dened inseveral equivalent ways :

asa weaklimitof Galton-Watson trees

through its height proess H, whih is a positive ontinuous proess on [0,1]. To a

point u ∈ [0,1] orresponds a vertex of the tree with height (distane to the root)

equaltoHu,andthemassmeasureonthetreeisrepresented byLebesgue'smeasure on[0,1]

through its expliit marginals, that is, the laws of subtrees spanned by a random

sampleof leaves.

We will have to use the seond (stohasti proess) and third (ombinatorial) points of

view. We know from the works of Duquesne and Le Gall [14℄ and Duquesne [13℄ that

one may denea partiular instane of tree, alled the stable tree with index α (for some α∈(1,2]).When α= 2, the stabletree is equalto the BrownianCRT of Aldous [2℄. We

willreall the rigorous onstrution of the height proess of the stable tree in Set. 2.2,

but let us state our results now. Fix α ∈ (1,2) and let (Hs,0 ≤ s ≤ 1) be the height

proess of the stable tree with index α.

The fragmentation proess, that we allF, is dened as follows. Foreah t ≥ 0, let I(t) be the open subset of (0,1)dened by

I(t) ={s∈(0,1) : Hs > t}.

Withour intuitive interpretation of the height proess, I(t) is the set of verties of the

tree with height > t. We denote by F(t) the dereasing sequene of the lengths of the

onneted omponents of I(t). Hene, F(t) is the sequene of the masses of the tree

omponentsobtainedby uttingthestable treebelowheightt.Notie thatF isadiret

generalization of the fragmentation F in [9, Setion 4℄. The boundedness of H implies

that F(t) = (0,0, . . .) as soonas t≥max0≤s≤1Hs.

Proposition 1 The proess F is a ranked self-similar fragmentation with index 1/α− 1∈(−1/2,0) and erosionoeient 0.

Notie that, as mentioned before, F loses some mass, and eventually disappears

ompletelyin nite time even thoughthe erosion is 0. This is due, of ourse, to the fat

that the self-similarityindex is negative.

Our main result is a desription of the disloation measure ν(ds) of F. Let us

introdue some notation. For α ∈ (1,2), let (Tx, x ≥ 0) be a stable subordinator with Laplaeexponent λ1/α, thatis,Tx isthe sum ofthe magnitudesofthe atomsofaPoisson

point proess on (0,∞) with intensity cαxdr/r1+1/α, where cα = (αΓ(1−1/α))−1. We

denoteby ∆Tx =Tx−Tx− the jump atlevelx and by ∆T[0,x] the sequene of the jumps

(5)

of T before time x, and ranked in dereasing order.Dene the measure να onS by να(ds) =E

T1; ∆T[0,1]

T1

∈ds

(1)

wherethelastexpression meansthatforanypositivemeasurablefuntionG,the quantity να(G) isequal to E[T1G(T1−1∆T[0,1])].

Theorem 1 The disloation measure of F isν =Dανα, where

Dα = α(α−1)Γ 1−α1

Γ(2−α) = α2Γ 2− α1 Γ(2−α) .

Someomments aboutthis. First,the disloationmeasure harges onlythe sequenes

sforwhih

P

i≥1si = 1,thatis,nomass anbelostwithinasudden disloation.Seond, wereognize anexpressionloseto[27℄,ofaPoisson-Dirihlettypedistribution.However,

it has to be notied that this orresponds to a forbidden parametrization θ = −1, and

indeed,the measure that we obtain is innitesine E[T1] = ∞. This measure integrates 1−s1 though,justasithasto.Indeed,E[T1−∆1]is niteif1 denotes thelargestjump

of T beforetime 1. To see this, notie that1 ≥∆1 where1 is a size-biased pik from thejumps of T beforetime 1,and itfollowsfrom Lemma1inSet.2.1belowand saling

arguments that T −∆1 has niteexpetation.

Therestof thepaperisorganizedasfollows. InSet.2werst reallsomefatsabout

Lévy proesses, exursions, and onditioned subordinators. Then we give the rigorous

desription of the stable tree, and state some properties of the height proess that we

will need. Last we reall some fats about self-similar fragmentations. We then obtain

the harateristis of F in Set. 3 and derive its semigroup. We insist on the fat that

knowing expliitly the semigroup of a fragmentation proess is in general a very om-

pliatedproblem, see [24℄ for somehow surprising negative results in this vein. However,

most of the fragmentation proesses that have been extensively studied in reent years

[3, 7, 22, 9℄ do have known, and sometimes strange-looking semigroups involving ondi-

tioned Poisson louds. And as a matter of fat, the fragmentation F+ onsidered in the

ompanion paper [23℄ has also anexpliit semigroup. We end the study of F by giving

asymptotiresults for smalltimes in Set. 4. These results need some properties of on-

ditionedontinuous-time branhing proesses,whihareinthe veinofJeulin's resultsfor

the resaled Brownian exursion and its loal times. We prove these properties in Set.

5, where we give the rigorous denition of some proesses that are used heuristially in

Set.3 to onjeture the form of the disloationmeasure.

2 Preliminaries

2.1 Stable proesses, exursions, onditioned inverse subordina-

tor

Throughout the paper, we let(Xs, s ≥ 0) be the anonial proess in the Skorokhod

spae D([0,∞)) of àdlàg paths on [0,∞). Reall that a Lévy proess is a real-valued àdlàg proess with independent and stationary inrements. We x α ∈ (1,2). Let P be

(6)

thelawthatmakesX astableLévyproesswithnonegativejumpsandLaplaeexponent E[exp(−λXs)] = exp(λα)fors, λ≥0,whereE istheexpetationassoiatedwithP.Suh

a proess has innite variationand satises E[X1] = 0. When there is noambiguity, we

may sometimes speak of X as being itself the Lévy proess with law P. Writing this in

the formof the Lévy-Khinthine formula, wehave :

E[exp(−λXs)] = exp

s Z

0

Cαdx

x1+α (e−λx−1 +λx)

, s, λ≥0, (2)

where Cα = α(α − 1)/Γ(2 − α). In partiular, the Lévy measure of X under P is Cαx−1−αdx1{x>0}. An importantproperty of X is then the salingproperty : under P,

1

λ1/αXλs, s≥0

= (Xd s, s≥0) for all λ >0.

It isknown [30℄ that under P, Xs has a density (ps(x), x∈R) for every s >0, suh that ps(x)is jointlyontinuous in xand s.

Exursions Let X bethe inmum proess of X,dened fors ≥0by Xs= inf{Xu,0≤u≤s}.

ByIt'sexursiontheoryforMarkovproesses,the exursionsawayfrom0ofthe proess X−X underP aredistributedaordingtoaPoissonpointproessthatanbedesribed by the It exursion measure, whih we all N. We now either onsider the proess X

underthelawP that makesitaLévy proessstartingat0,orunderthe σ-nitemeasure N under whih the sample paths are exursions with nite lifetime ζ (sine E[X1] = 0).

LetN(v)bearegularversionoftheprobabilitylawN(·|ζ =v),whihisweaklyontinuous

inv. That is,for any positiveontinuous funtional G, N(G) =

Z

(0,∞)

N(ζ ∈dv)N(v)(G)

andlimN(w)(G) = N(v)(G)asw→v.Suhaversionan beobtainedbysaling:forany

xed η >0,the proess

(v/ζ)1/αXζs/v,0≤s ≤v

under N(·|ζ > η) = N(·, ζ > η) N(ζ > η)

isN(v). See [12℄ for this and other interesting ways to obtain proesses with lawN(v) by

pathtransformations.Inpartiular,onehasthesalingpropertyatthelevelofonditioned

exursions : under N(v), v−1/αXvs,0≤s≤1

has law N(1).

First-passage subordinator Let T be the right-ontinuous inverse of the inreasing proess −X,that is,

Tx = inf{s≥0 :Xs<−x}.

Then itis known that underP, T isa subordinator, that is, aninreasing Lévy proess.

Aording to [6, Theorem VII.1.1℄, its Laplae exponent φ is the inverse funtion of the

(7)

restrition of the Laplae exponent of X to R+. Thus φ(λ) = λ1/α, and T is a stable

subordinator with index 1/α,as dened above. The Lévy-Khinthine formulagives,

E[exp(−λTx)] = exp(−xλ1/α) = exp

x Z

0

cαdy

y1+1/α(1−e−λy)

for λ, x≥0.

where cα has been dened in the introdution. Reall our assumption that X has a

marginaldensity attimes under P,alledps(·). Thenunder P,the inverse subordinator

T has also biontinuous densities, given e.g. by [6,Corollary VII.1.3℄:

qx(s) = P(Tx ∈ds)

ds = x

sps(x). (3)

This equationan bederived fromthe ballottheorem of Takás [31℄.

Let usnow disuss the onditioned forms of distributions of the sequene ∆T[0,x]. An

easywaytoobtainnie regularversionsfortheseonditionallawsisdeveloped in[25,27℄,

and uses the notion of size-biased fragment. Preisely, the range of any subordinator,

with drift 0 say (whih we will assume in the sequel), between times 0 and x, indues

a partition of [0, Tx] into subintervals with sum Tx. Consider a sequene (Ui, i ≥ 1) of

independent uniform (0,1) variables, independent of T, and let1(x),∆2(x), . . . be the

sequene ofthe lengthsof theseintervalsinthe orderinwhihthey are disovered by the

Ui's.That is,1(x) is the length of the interval in whih TxU1 falls,2(x) is the length

ofthe rst intervaldierent fromthe one ontaining TxU1 inwhihTxUi falls,and soon.

ThenPalmmeasureresults forPoissonloudsgivethefollowingresult(speializedtothe

ase of stablesubordinators).

Lemma 1 The joint law under P of (∆1(x), Tx) is

P(∆1(x)∈dy, Tx ∈ds) = cαxqx(s−y)

sy1/α dyds, (4)

and more generally for j ≥1, P ∆j(x)∈dy

Tx =s0,∆1(x) =s1, . . . ,∆j−1(x) =sj−1

= cαxqx(s−y) sy1/αqx(s) dy,

where s=s0−s1−. . .−sj−1.

This gives a nie regular onditional version for (∆i(x), i ≥ 1) given Tx, and thus

induesaonditionalversionfor∆T[0,x]givenTx,byranking,where∆T[0,x]isthesequene

of jumps of T beforex, ranked in dereasing order of magnitude.

2.2 The stable tree

Wenowintroduethemodels oftreeswe willonsider. Thissetionismainlyinspired

by [14, 13℄. With the notations of setion 2.1, for u ≥ 0, let R(u) be the time-reversed proess of X attime u :

R(u)s =Xu−X(u−s)− , 0≤s≤u.

(8)

Itis standard that this proess has the same lawas X killed attime uunder P.Letalso R(u)s = sup

0≤v≤s

R(u)v , 0≤s≤u

be its supremum proess. We let Hu be the loal time at 0 of the proess R(u) reeted

underits supremum R(u) up totime u. The normalizationan behosen sothat

Hu = lim

ε↓0

1 ε

Z u 0

1{R(u)s −R(u)s ≤ε}ds

It is known by [14, Theorem 1.4.3℄ that H admits a ontinuous version, with whih we

shall work in the sequel. It has to be notied that H is not a Markov proess (the only

exeptioninthe theory of Lévy trees isthe Brownian treeobtained when P isthe law of

Brownian motion with drift, whih has been exludedin our disussion). As a matter of

fat,it an beheked that H admits loalminima that are attained aninnite number

of times as soon as X has jumps, a property that sounds strange by ontrast with most

ofthe usually studied stohasti proesses.Tosee this, onsider ajumptime t of X, and

lett1, t2 > t so thatinft≤u≤tiXu =Xti and Xt− < Xti < Xt,i∈ {1,2}.Then itis easyto

see that Ht=Ht1 =Ht2 and that one may infat nd aninnite number of distint ti's

satisfyingthe propertiesof t1, t2. On the other hand,it is not diultto see that Ht isa

loalminimumof H.

Itisshownin[14℄thatthe denitionofH stillmakessense undertheσ-nitemeasure N rather than the probability law P. The proess H is then dened only on [0, ζ], and

weallit the exursion of the height proess. One an dene withoutdiulty, using the

salingproperty, the height proess underthe laws N(v) :this is simplythe lawof v

ζ

1−1/α

Hζt/v,0≤t≤v

!

underN(·, ζ > η)

Callitthelawoftheexursionoftheheightproesswithdurationv.Thefollowingsaling

property is the key for the self-similarityof F : for every x >0,

(v1/α−1Hsv,0≤s≤1)under N(v) = (Hd s,0≤s≤1)under N(1). (5)

This property is inherited from the saling property of X, and it is easily obtained e.g.

by the above denition of H asan approximation.

An important tool for studying the height proess is its loal time proess, or width

proess, whih wewilldenote by (Lts, t≥0, s≥0). It an be obtained a.s. for every xed s, tby

Lts= lim

ε↓0

1 ε

Z s 0

1{t<Hu≤t+ε}du.

Ltsisthenthe densityofthe oupationmeasure ofH atlevelt andtimes.Fort= 0,one

hasthat(L0s, s≥0)isthe inverse ofthesubordinatorT,whihisareminisentofthefat

thattheexursions oftheheightproessareinone-to-oneorrespondenewithexursions

of X with the same lengths.Aording to the Ray-Knight theorem [14, Theorem 1.4.1℄,

for every x > 0, the proess (LtTx, t ≥ 0) is a ontinuous-time branhing proess with

Références

Documents relatifs

Self-similar fragmentations derived from the stable tree II: splitting at nodes..

Given a general critical or sub-critical branching mechanism and its associated L´evy continuum random tree, we consider a pruning procedure on this tree using a Poisson snake..

K´ arm´ an’s flows on a single and between two infinite coaxial rotating disks are famous examples of self-similar solutions of the Navier–Stokes equations.. Consi- dering

supposing that the (ϕ k ) 0≤k≤N are strict contractions, we prove a partial extension of the theorem of Erd¨ os [4], showing that for most parameters in the small island the

The proof in Section 5.1 shows that we loose quite much information when applying Sgibnev’s result (see Proposition 6.1 in Appendix) on the kew renewal theorem for a random walk

Existence of mass-conserving self-similar solutions with a sufficiently small total mass is proved for a specific class of homogeneous coagulation and fragmentation coefficients..

Lamb, Existence and uniqueness results for the continuous coagulation and fragmentation equation, Math..

The only sssi Gaussian process is the fractional Brownian motion; however there are many different sssi symmetric stable processes, which often arise in limit theorems for the