A NNALES DE L ’I. H. P., SECTION B
D AYUE C HEN
Average properties of random walks on Galton-Watson trees
Annales de l’I. H. P., section B, tome 33, n
o3 (1997), p. 359-369
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359
Average properties of random
walks
onGalton-Watson trees
Dayue
CHENDepartment of Probability and Statistics
Peking University, Beijing, 100871, China.
Vol. 33, n° 3, 1997, p. 369. Probabilités et Statistiques
ABSTRACT. - We
study
the A-biased random walk on Galton-Watson treesby
the Dirichletprinciple
and a formula of mean exit time of a Markov chain. We prove that the average ofescaping probability
and mean exittime are bounded
by
thecounterparts
of thecorresponding
random walkson {0,1,2,’’’ - - -}.
Inparticular
wepartially
verified the recentconjecture
of
Lyons,
Pemantle and Peres on the upper bound of thespeed
of A-biasedrandom walk on Galton-Watson trees.
RESUME. - Nous etudions la marche aleatoire de biais A sur un
arbre de Galton-Watson. Nous demontrons que la
probability
de fuiteet le
temps
de sortie en moyenne sont bornes par ceux de la marche aleatoirecorrespondante sur {0,1,2, " - " ’}.
Enparticulier
nous confirmonspartiellement
uneconjecture
deLyons,
Pemantle et Peres sur la limitesuperieure
de vitesse de la marche aleatoire de biais A sur un arbre de Galton-Watson1. INTRODUCTION
For a
given
treeT,
a vertex is selected as the root and is denotedby
o.Supported in part by a grant from the NSF of China.
Annales de l’Institut Henri Poincaré - Probabilités et Statistiques - 0246-0203
The distance from vertex v to o is the minimum number of
edges linking
o
and v,
and is denoted It is called the level orgeneration
of v.For vertex v other than root o
(i . e, I
>0),
there is aunique adjacent
vertex which is of
level
1. Thisunique adjacent
vertex is called the parent of v, and is denotedby
~4. Otheradjacent
vertices of v are all oflevel |v|
+1,
and are called children of v.Let kv
be the number of children of v. It is also known as thebranching
number of v. Children of v aredenoted
by
uz, i =1,2,-"~.
For
positive
numberA,
~-biased random walk on T is a Markov chain~Xn ~
on the vertices of T with transitionprobability
The transition
probability
at o is differentslightly
in accordance with the lack of o* .Let ko
be thebranching
number of o and °i a child of o. We definep ( o, oi )
=1 / I~o
in addition to( 1 ).
Note that( 1 )
is also well defined for A = 0 ifkv
> 1 for all vertices v’s of T. LetTree T is called a Galton-Watson tree if it is a realization of a Galton- Watson process.
Namely, kv’s
are i.i.d. random variables. Assume that theoffspring
distribution satisfies thatThe
offspring
distribution inducesnaturally
aprobability
measure in thecollection T of all Galton-Watson trees. Let
ET
be theexpectation according
to that
probability
measure on T. DefineCertainly
m’>
1. ~-biased random walk on random trees is defined in twosteps. First,
take a Galton-Watson tree Taccording
to theprobability
measure in T.
Then,
define a random walkXn
on Taccording
to( 1 ) starting
Annales de l’Institut Henri Poincaré - Probabilités et Statistiques
at root o. Thus a
point
in thebig probability
space has twocomponents:
a random tree and a randompath.
Theoffspring
distribution andparameter A
determine a
unique probability
measure in thisbig
space. In thefollowing
Theorem
2,
the doubleexpectation ET E
is the average first over all random walks on a fixed treestarting
at root o, then over all Galton-Watson trees.The
equalities
holdif
andonly if
m =m’, i.e.,
m is aninteger
andP(k
=m)
= 1.THEOREM 2. - Assume that
P(k
=0)
= 0. ThenThe
equalities
holdif
andonly if
m =m’, i.e.,
m is aninteger
andP(l~ = m) =
1.Random walk on random trees has been an active
subject
in recentyears. It is shown in
[4]
that the random walk on random trees is transienta. s . in the
big
space if A m. Thespeed,
or the rateof
escape, of the random walk is defined to beliminfn~~ Xn’ /n. Lyons,
Pemantle and Peresproved recently
in[5] ]
that for a fixed A(A m )
and for a.e.Galton-Watson tree
T,
. exists and is a
positive
constant, denotedby speed(~). speed(~) depends only
on A and theoffspring
distribution. For the case A =1, they computed
the
speed explicitly
in[6].
On the other
hand,
consider the random walkon {0,1,2,3,’"} (which
isthe
simplest tree)
with thefollowing
transitionprobabilities.
3-1997.
One can
easily verify
thatspeed(A) = (m -
+A)
in this case.Comparing
with(7)
we see that when A = 1 the random walk on random trees is slower than thecorresponding
random walk on{0,1,2,3, - "}.
It isoften observed that a random walk is slowed down in random environments.
A related
example
can be found in[8].
It isconjectured
in[7]
thatWe are motivated
by
thisconjecture,
andverify
itpartially.
COROLLARY 3. - =
0 ) = 0, ~
1 and m 00, thenThe
equality
holdsif
andonly if
m =m’, i.e., P(k
=m)
= 1for
someinteger
m.By (7)
and theconvexity
of function(x - 1 ) / (x
+1 ), Corollary
3 holdsfor 03BB = 1. For 03BB
1,
one can showby coupling
that s is bounded aboveby
that of a random walk on~0, 1,2,3, ...}
with transitionprobabilities
Hence
Ts /s
isuniformly integrable
in thebig
space.By Proposition
5.112of
[ 1 ],
we canexchange
theintegration
and thelimit, i . e .,
the lastequality,
in the
following
derivation.The
corollary
now follows from Theorem 2. The next two sections aredevoted to the
proof
of Theorems 1 and 2respectively.
2. PROOF OF THEOREM 1
For
computing P(Ts To IXo
=o)
on a fixed Galton-Watson treeT,
it suffices to consider the subtree ofgenerations 0, 1, 2, ... , s
of T. Ondefine a random walk
~Xn ~ according
toAnnales de l’Institut Henri Poincaré - Probabilités et Statistiques
Then the random walk so defined is reversible in the sense
.
x)
for any vertices x, y(not necessarily adjacent)
ofT,
andLet H be the collection of all functions h on the vertices of such that
Then, by
the Dirichletprinciple (page
99 of[3]),
Consequently,
Upper
bound. Define thedecreasing
sequenceTake h E H such that
h(x)
= ThenVol. 33, n° 3-1997.
Since
P(Ts o|X0
=o)
isdecreasing
in s, converges to03B3(T),
and isbounded,
Lower bound. Given a tree
T,
consider thesimple forward
random walk which choosesrandomly (uniformly)
among the children of the presentvertex as the next vertex. Let
~c(x)
be theprobability
that the random walkstarting
at root o will visit vertex x. Ifkix’ s
are thebranching
numbers of the vertices
along
the shortestpath
from root o to x, then~(~r)
=l~x~ )-l.
This is thevisibility
measure of the set of raysemanating
from root o andpassing
vertex x. See§2
of[6]
for the details.By
theCauchy-Schwarz inequality,
for any hE H,
Since
~~-1 ~(~) = ~(~),
theright
hand side of the aboveinequality actually
isequal
toThus
by (10),
Annales de l’lnstitut Henri Poincaré - Probabilités et Statistiques
and
Letting s
- oo we obtain the other half of Theorem 1. D It is shown in theproof
ofCorollary
3.5 of[5]
thatwhere qx is the smallest
nonnegative
numbersatisfying
The lower bound of Theorem 1 is
simpler
and works better when ~ l.is called the
escaping probability.
If tree T isthought
as an electricalnetwork,
and if the resistance of anedge linking
vertices of level l and(l -i-1 )
is
~l,
then the total resistance between vertex o and theinfinity
isIn
deriving
the lower bound weactually proved
astronger
statement.COROLLARY 4. -
If P(k
=0)
= 0 and 03BB m’ oo, then the total resistance between root o and theinfinity
has afinite
mean over allGalton-Watson trees.
Namely,
3. PROOF OF THEOREM 2
Choose l E
[0, s].
Take the subtree of the first l levels of a Galton- Watson tree and extend itby pipes .(see Figure).
In our earlier notation the tree is characterizedby kv
= 1for I v I
> l . The collection of all such infinite trees withpipes
at level l is denotedby T(l).
Theoffspring
distribution induces a
probability
measure onT(l)
for every l . In thefollowing
Lemma5, ET(l)
is theexpectation
taken withrespect
to thisVol. 33, n° 3-1997.
induced measure on
T(I). Restricting
attentiononly
to the first Ilevels,
a subset of
T(I)
can beregarded
also as a subset ofT( I
+1)
and it has the sameprobability
measure in bothT(l)
andT(l +1).
This consistence of induced measures onT(l)’s
is used in theproofs
of Lemma 5 and Theorem 2 below.Run a random walk on T E
T(l)
with transitionprobabilities
Some obvious
change
is needed if l = 0 or v = o. LetExTs
be the meanof the first
hitting
time of level sby
the random walk definedby ( 11 ) starting
at vertex x.Proof
1 .1. -Suppose
that tree T’ ET ( + 1).
Thatis,
from level(I + 1 )
on there is
only
one child for each vertex.Suppose
that u is a vertex of = Iand ku
is thebranching
number of u. Notice that thereare
ku pipes emanating
from u and the transitionprobabilities along
thesepipes
are identical. So we combine thesepipes together
as one combinedAnnales de l’lnstitut Henri Poincaré - Probabilités et Statistiques
pipe.
Let ui be theonly
child of u after thiscombination,
andchange
thetransition
probability
at u asThe randomness of the
branching
number of u is converted to the randomness of transitionprobability
at The distributionof s
ispreserved
after this modification. In
particular,
we haveIn
general
Replacing (13) by
and
solving
thesystem
of linearequations by
the Cramerrule,
we see thatEoTs
is thequotient
of two determinants. Notice that appearsonly
inthe last
equation.
Thus each determinant is a linear function ofku
andwhere a, b,
c and d areindependent
ofFunction
/(~c) = (ax-~-b)/(cx-~-d)
is convex if andonly
iff(0)
>f {oo).
However, f(O)
isEoTs when ku
=0,
or in otherwords, p(u, ui)
=0, p(u, u* )
=1;
and,f {oo)
isEoTs
when =1, p(u, u* )
= 0. Definetwo random walks
~Yn ~
bothstarting
at root o, with the sametransition
probability everywhere except
at u. For{Y~}.
=0, p(u, u* )
=1;
=1, p(u, u* )
= 0. Notice that the combinedpipe
and otherpipes
of the tree aresymmetric beyond
levelVol. 33, n° 3-1997.
(l
+1), including
level(l
+1).
SoIZnl by
the method ofcoupling.
It is follows from this fact that
f (0)
>f (x) (unless s
=1).
We have demonstrated that
EoTs
is a convex function ofBy
theJensen’s
inequality,
the average ofEoTs
over allpossible k~
isgreater
thanor
equal
to(am
+6)/(cm
+d).
This isexactly
the meanhitting
time oflevel s
by
the random walk with deterministic transitionprobability
at u,The above
argument
can beapplied
to other vertices of level loneby
one to decrease the mean
hitting
time of level s. What we haveproved
isthat for T E
T(l), EoTs
is less than orequal
to the average ofEoTs
overthose trees of
T(
+1 )
whose subtree of first l levels is T. Theequality
holds if and
only
ifP(k
=m)
= 1 for someinteger
m. The statement ofthis lemma then follows
by taking
the average of random trees ofT(l).
Namely,
takeET(l) .
DRemark. - This
simplied proof
iskindly suggested
to the authorby
Professor R.
Lyons.
Theoriginal proof
islengthy
and uses a cumbersomeformula of the mean exit time from
[2].
Proof of
Theorem 2. - The distribution of firsthitting
time TS of level sis determined
by
the subtree of first s levels.By
the consistence of inducedmeasures on
T ( s )
andT,
andby
Lemma5,
we have thatETETs
=ET(s)EoTs 2: (15)
However,
there isonly
one member ofT(0).
Theright
hand side of(15)
further reduces to the mean of the first
hitting time Ts
of sby
therandom walk
on {0,1,2,3,---} starting
at 0 with transitionprobabilities given by (8).
This can be calculatedby solving
asystem
of linearequations.
The first half of Theorem 2 is now an easy consequence of
(15)
and(16).
For the second
half,
rewrite(14)
aswhich is a concave function of
Taking
the average overI~y
weget
The
remaining argument
is identical with that of the first half. DAnnales de l’Institut Henri Poincaré - Probabilités et Statistiques
Remark. - It is for
simplicity
that we assumethroughout
this paper thatP(k
=0)
= 0. Thisassumption
is needed in the halfinvolving m’
of boththeorems;
but is notrequired
for the other half(involving m).
ACKNOWLEDGMENTS
The author would like to thank Professor Y. Peres for
private
communications and
encouragement,
and Professor R.Lyons
for valuablecomments that
simplify greatly
theproof
of Lemma 5. This work is done while the author isvisiting
UCLA. The author wishes to thank Professor TomLiggett
for hishospitality,
and for discussions related to this research.REFERENCES [1] L. BREIMAN, Probability, SIAM, Philadelphia, 1992.
[2] D. CHEN, J. FENG and M. P. QIAN, The metastability of exponentially perturbed Markov chains, Science in China, Vol. 39, 1996, pp. 7-28.
[3] T. M. LIGGET, Interacting Particle Systems, Springer-Verlag, New York, 1985.
[4] R. LYONS, Random walks and percolation on trees, Ann. Prob., Vol. 18, 1990, pp. 931-958.
[5] R. LYONS, R. PEMANTLE and Y. PERES, Biased random walks on Galton-Watson trees,
Probability Theory and Related Fields, Vol. 106, 1996, pp. 249-264.
[6] R. LYONS, R. PEMANTLE and Y. PERES, Ergodic theory on Galton-Watson trees: speed of
random walk and dimension of harmonic measure, Ergod. Th. & Dynam. Sys., Vol. 15, 1995, pp. 1-27.
[7] R. LYONS, R. PEMANTLE and Y. PERES, Unsolved problems concerning random walks on trees.
In "Classical and Modem Branching Processes", K.B. Athreya and P. Jagers (editors), Springer-Verlag, New York, 1996, pp. 223-238.
[8] F. SOLOMON, Random walk in a random environment, Ann. Prob., Vol. 3, 1975, pp. 1-31.
(Manuscript received January 7, 1996;
Revised March 4, 1996. )
Vol. 33, n° 3-1997.