This paper proves that the tributary structure of Howard's drainage model, conditioned on survival, converges to a continuum random tree, confirming a prediction by Aldous using a Brownian web approach.
Contribution
It establishes the convergence of scaled tributary structures to a continuum random tree using dual processes and Brownian web techniques, extending prior predictions.
Findings
01
Scaled tributaries converge to a continuum random tree
02
The limiting tree differs slightly from earlier predictions
03
Dual process convergence to Brownian web is key
Abstract
We consider the tributary structure of Howard's drainage model studied by Gangopadhyay et. al. Conditional on the event that the tributary survives up to time n, we show that, as a sequence of random metric spaces, scaled tributary converges in distribution to a continuum random tree with respect to Gromov Hausdorff topology. This verifies a prediction made by Aldous for a simpler model (where paths are independent till they coalesce) but for a different conditional set up. The limiting continuum tree is slightly different from what was surmised earlier. Our proof uses the fact that there exists a dual process such that the original network and it's dual jointly converge in distribution to the Brownian web and it's dual.
Equations272
h(x,t):=⎩⎨⎧(x+k0,t+1)(x−k0,t+1)(x+U(x,t)k0,t+1) if B(x−k0,t+1)∈/V if B(x+k0,t+1)∈/V otherwise.
h(x,t):=⎩⎨⎧(x+k0,t+1)(x−k0,t+1)(x+U(x,t)k0,t+1) if B(x−k0,t+1)∈/V if B(x+k0,t+1)∈/V otherwise.
min(x,t):=mout(x,t):=ϵ↓0lim{number of paths in W starting at (y,t−ϵ) for some y that pass through (x,t) and are disjoint in the time interval (t−ϵ,t)};ϵ↓0lim{number of paths in W starting at (x,t) that are disjoint in the time interval (t,t+ϵ)}.
min(x,t):=mout(x,t):=ϵ↓0lim{number of paths in W starting at (y,t−ϵ) for some y that pass through (x,t) and are disjoint in the time interval (t−ϵ,t)};ϵ↓0lim{number of paths in W starting at (x,t) that are disjoint in the time interval (t,t+ϵ)}.
θ0:=inf{θ1:=t≥0: there exists π1∈W such that σπ1=t,π1(t)=π0(t) and π1(t+1)=π1(t+1)},γ(π0,π1).
θ0:=inf{θ1:=t≥0: there exists π1∈W such that σπ1=t,π1(t)=π0(t) and π1(t+1)=π1(t+1)},γ(π0,π1).
(π+(s),π−(s)):={(π0(θ0+s)−π0(θ0),π1(θ0+s)−π0(θ0))(π1(θ0+s)−π0(θ0),π0(θ0+s)−π0(θ0)) if π0(θ0+1)>π1(θ0+1) if π0(θ0+1)<π1(θ0+1).
(π+(s),π−(s)):={(π0(θ0+s)−π0(θ0),π1(θ0+s)−π0(θ0))(π1(θ0+s)−π0(θ0),π0(θ0+s)−π0(θ0)) if π0(θ0+1)>π1(θ0+1) if π0(θ0+1)<π1(θ0+1).
(π+,π−)=d(B+,B−),
(π+,π−)=d(B+,B−),
(B1/n,B0)∣{γn≥1}⇒(B+,B−).
(B1/n,B0)∣{γn≥1}⇒(B+,B−).
λ0(f1,f2):=inf{λ1(f1,f2):=inf{t≥0:(f1(s1)−f2(s1))(f1(s2)−f2(s2))>0 for all s1,s2∈(t,t+1)} and t>λ0:f1(t)=f2(t)}.
λ0(f1,f2):=inf{λ1(f1,f2):=inf{t≥0:(f1(s1)−f2(s1))(f1(s2)−f2(s2))>0 for all s1,s2∈(t,t+1)} and t>λ0:f1(t)=f2(t)}.
λ0n(f1,f2):=inf{
λ0n(f1,f2):=inf{
for all s1,s2∈(t,t+1)} and
λ1n(f1,f2):=inf{
A:={
A:={
An:={
Peer Reviews
No public reviews on file for this paper yet. If you reviewed it on a platform where reviews are public (OpenReview, ICLR, NeurIPS, ICML), you can paste yours below so the community can read it here.
Videos
No videos yet. Explain this paper in a talk, walkthrough, or lecture? Add one.
Taxonomy
TopicsStochastic processes and statistical mechanics · Theoretical and Computational Physics · Bayesian Methods and Mixture Models
Full text
Continuum random tree as the scaling limit for a drainage network
model: a Brownian web approach
Kumarjit Saha111Ashoka University
222This work is benefited from the support of the AIRBUS
Group Corporate Foundation Chair in Mathematics of Complex Systems established in ICTS-TIFR
and supported in part by ISF-UGC grant.
Abstract
We consider the tributary
structure of Howard’s drainage network model studied by Gangopadhyay et al. [13].
Conditional on the event that the tributary survives up to time n, we show that, as a sequence of random metric spaces, scaled tributary converges in distribution to a continuum random tree with respect to Gromov Hausdorff topology.
This verifies a prediction made by Aldous [3] for a simpler model (where paths are independent till they coalesce) but for a different conditional set up. The limiting continuum random tree is slightly different from what was surmised in
[3]. Our proof uses the fact that there exists a dual process such that the original network and it’s dual jointly converge to the Brownian web and its dual. The limiting continuum random tree is universal in the sense that for all discrete drainage network models with non-crossing paths
in the basin of attraction of the Brownian web, the conditional scaled tributaries converge to the same scaling limit.
Keywords: Continuum random tree, Gromov-Hausdorff distance, coalescing random
walk, Brownian web.
AMS Classification: 60D05
1 Introduction
Trees are often used to represent genealogical structures,
communication network modelling, optimisation and
river basin study. During the last three decades there has been an interest in
understanding the scaling limits of various discrete random trees.
Most notably in [2], Aldous showed that an appropriately scaled Galton-Watson tree with a finite variance critical offspring distribution and conditioned to have total population size n, as n→∞, converges to a continuum random tree (CRT) famously known as the Brownian CRT. In the recent years, these results have been extended for more general continuum random trees (e.g., see [20]).
These concepts and results have found
many other applications also, e.g., understanding the scaling limits for thhe sequence of components
of critical Erdos-Renyi random graph ([4], [5]). Further this
limiting behaviour appear to be universal in the sense that Aldous’ limiting picture for
critical random graph has since been extended to “immigration” models of random graphs
[6], hypergraphs [12] and to random graphs with fixed degree [23].
In this paper we show that a sequence of appropriately scaled discrete trees obtained from a drainage network model converge in distribution to a continuum random tree which is different from the Brownian CRT.
Various statistical models of drainage networks have been proposed (see [24] for a detailed survey). In this paper, we
study the ‘tributary’ tree of a two-dimensional drainage network called
the Howard’s model of headward growth and branching [14].
In order to present our result, we first describe Howard’s network model. Fix p∈(0,1) and let {Bu:u=(u(1),u(2))∈Z2} be an i.i.d. collection of Bernoulli random variables with success probability p. In what follows, a vertex (x,t) with B(x,t)=1 will be called as an open vertex. Let {Uu:u∈Z2} be another collection of random variables, independent of the collection {Bu:u∈Z2} taking values 1 and −1 with equal probabilities. For (x,t)∈Z2, let k0:=min{∣k∣:k∈Z,B(x+k,t+1)=1} and we define
[TABLE]
This gives a random graph G with vertex set V:={u:Bu=1}, i.e., the set of open vertices, and
edge set E:={⟨(x,t),h(x,t)⟩:(x,t)∈V}. In other words, each open vertex connects to the nearest open vertex at the next level and in case of ties, chooses one of them uniformly independent of everything else. This gives a stochastic drainage network model, where each open vertex acts as a source vertex and from each open vertex (x,t), water comes out and flows to h(x,t) along the channel given by the edge ⟨(x,t),h(x,t)⟩. Clearly by construction, G does not have a cycle or loop almost surely.
Gangopadhyay et al. [13] studied this random graph in detail and showed the following:
Theorem 1.1**.**
G* is connected and there is no bi-infinite path in G almost surely.*
It should be mentioned here that, Gangopadhyay et al. [13] studied this model for Zd with d≥2 and observed
a tree-forest dichotomy behaviour depending on dimensions. In this paper, we are interested about d=2 only and the construction that we mentioned here is different from that of [13] but
generates the same process for d=2.
For k≥1 and for (x,t)∈Z2, let hk(x,t)=h(hk−1(x,t)) with h0(x,t)=(x,t).
For (x,t)∈Z2,
we now define the cluster or the tributary at (x,t) (see Figure 1),
consisting of all the source vertices whose water flows through (x,t), as
[TABLE]
The set of edges in cluster C(x,t) is denoted by
[TABLE]
We consider R2 as space-time plane, i.e, space and time are measured along X axis and Y axis respectively. The ‘depth’ of the cluster C(x,t), i.e., the time length that the cluster survived
(see Figure 1), is defined as
[TABLE]
For any set A, we define #A to be the cardinality of A. It follows from Theorem 1.1 that both the random variables, #C(x,t) and L(x,t), are finite almost surely.
We consider the tree T(x,t) obtained from the sub-graph (C(x,t),E(x,t)) with the natural graph metric. For n≥1,
Tn(x,t) denotes the scaled tree where distances are scaled by 1/n.
More formally, let
[TABLE]
denote the discrete
weighted tree formed by the cluster C(x,t),
the edge set E(x,t) and the weight function 1, where 1 attaches costant weight 1 to each edge in E(x,t). For n≥1
let Tn(x,t):=(C(x,t),E(x,t),1n) denote the scaled tree where
1n(e)=1/n for all e∈E(x,t). For each n≥1, the random object Tn(x,t) can be regarded as a random metric space where the distance between any two vertices (in C(x,t)) is given by the sum of the edge weights along the unique path between them. Note that the distribution of Tn(x,t) does not depend on the vertex (x,t)∈Z2.
The main result of this paper is that, the conditional distribution of Tn(0,0) given that {L(0,0)≥n} converges to a continuum random tree as n→∞. In order to state our result we need to describe the relevant topology briefly.
Gromov-Hausdorff topology is a common way to define a topology (even a metric)
on a space of compact metric spaces. This had been introduced by Gromov [21].
For any two compact subsets K and K′ of a metric space (X,d), the
Hausdorff distance dH(K,K′) is given by:
[TABLE]
where for ϵ>0, the set Kϵ is defined as
Kϵ:={x∈X:d(x,K)≤ϵ}.
The Gromov-Hausdorff distance between two compact metric spaces (X,d) and (X′,d′) is defined by
[TABLE]
where infimum is taken over
all possible choices of isometric embeddings ϕ,ϕ′ of the metric spaces (X,d) and (X′,d′) into a common metric space.
Let M be the set of all isometry equivalence classes of compact metric spaces endowed with the Gromov-Hausdorff metric.
It is known that this distance turns M
into a Polish space.
We mention here that given a metric space (X,d), we write
[X,d] to denote the isometry equivalence classes of (X,d),
and frequently use the notation X for either (X,d) or [X,d] when there is no risk of ambiguity.
We show that as n→∞, the conditional distribution of Tn(0,0) given {L(0,0)>n} converges to a continuum random tree, which we denote by T.
Throughout this paper the notation ⇒ is used to denote convergence in distribution.
Theorem 1.2**.**
As n→∞, we have
[TABLE]
where convergence in distribution holds with respect to the Gromov-Hausdorff topology on M.
We comment that the limiting continuum random tree T is different from the Brownian CRT and to the best of our knowledge this limiting tree has not been studied earlier in the literature.
In the next section, we construct T and explain the difference of T from the one that was surmised in [3].
Slightly related random tree has been studied in [27]. In Section 5 we mention about the work in [27] in more detail.
We don’t have the complete understanding of the limiting object T yet. Most notably
we do not know what is the distribution of the contour walk of T as a process (see Section 5 for more details).
Scaling of conditioned tributaries are of importance because of their relations with different scaling laws empirically observed for river networks. Regarding this, we should mention that the conditional tributary for Howard’s model was studied earlier and it was proved that the joint distribution of (L(x,t),(#C(x,t))) has a regularly varying tail (Theorem 1.4 [29]). In order to describe another result for conditional tributary, let us describe another drainage network model.
Let Zeven2:={(x,t):x,t∈Z,x+t even}
be the oriented lattice. Each (x,t)∈Zeven2 acts as a source, and starting from spatial location x at time t water flows to location (x+1) or (x−1) at time t+1 with equal probability.
Formally, consider {b(x,t):(x,t)∈Zeven2}, a collection of
i.i.d. random variables taking values +1 and −1 with equal probabilities.
For (x,t)∈Zeven2, let hRW(x,t):=(x+b(x,t),t+1)
and for k≥1, k-th step is given by hRWk(x,t):=hRW(hRWk−1(x,t)) where hRW0(x,t)=(x,t).
For (x,t)∈Zeven2, we observe that
the process {hRWk(x,t)(1):k≥0}
is a one-dimensional simple symmetric random walk starting from location x
at time t. Hence the random graph formed by the vertex set Zeven2
and the edge set E:={⟨(x,t),hRW(x,t)⟩:(x,t)∈Zeven2} may be viewed as a graphical representation of a system of 1-dimensional coalescing simple symmetric random walks starting from every point of Zeven2. This is known as Scheidegger’s model of drainage network [30].
For (x,t)∈Zeven2,
the tributary CRW(x,t) and its depth LRW(x,t) are defined similarly
as in the case of Howard’s model. Nguyen proved the following (Theorem 1 of [22]):
Theorem 1.3**.**
There exists c>0 such that
[TABLE]
Clearly, Scheidegger’s model has no cycle and in a similar way we can consider TRW(0,0), which is the subtree obtained from the vertices {(x,t)∈Zeven2:t≥0} and the associated edges lying in the connected component of (0,0) with the usual graph distance. For n≥1, let TnRW(0,0) denote the scaled tree where distances are scaled by 1/n.
Aldous predicted that the conditional distribution of TnRW(0,0) given that {LRW(0,0)=n}
converges to a CRT as n→∞ (see Subsection 4.2 Page 275 of [3]). With a modification, [3]
also provides fairly accurate description of the limiting CRT. In the same paper in Section 3, Aldous provided
finite dimensional convergence conditions and a tightness condition as a tool to study convergence to a continuum random tree.
Specifically for the (predicted) scaling limit of conditional tributary coming from Scheidegger’s model, he further commented that:
“It is intuitively clear that rescaling the edges of TnRW(0,0) by 1/n, these random trees converge to the continuum random tree defined as above ⋯. This could be proved using the ideas of Nguyen [22] and Section 3.”
Though the above comment suggests that finding the scaling limit is trivial in this case, but there are some important issues which we now try to highlight.
Long before, Arratia [1] observed that the system of coalescing simple symmetric random walks starting from every point on the oriented lattice has a natural dual represented by coalescing simple symmetric random walks starting from every point on Zodd2:={(x,t)∈Z2:x+t odd } progressing in the backward direction of time (see Figure 2).
To the best of our knowledge, Nguyen was the first to observe that survival of CRW(0,0) can be studied through coalescence of the dual random walks starting from (−1,0) and (1,0).
The dual random walks starting from (1,0) and (−1,0) are independent till
they meet. This property of independence till the time of coalescence, which is very specific
to this model, allowed Nguyen to use the following functional limit theorem of Kaigh [17]
to prove the result.
Theorem 1.4**.**
Random walk excursion converges to the Brownian excursion.
The above theorem is central in establishing Theorem 1.3. Now going back to the question of finding the metric space limit of TnRW(0,0), in order to obtain fnite dimensional convergences, we should observe that, given {LRW(0,0)=n}, the subtrees spanned by the uniformly picked vertices from the cluster CRW(0,0), are no longer given by simple random walk paths and one has to prove a suitable version of Theorem 1.4, which is a considerable tusk. More importantly, while dealing with models where paths are no longer independent and have interactions, e.g., Howard’s model, Nguyen’s method does not help.
Roy et al. [29] showed that there exists a dual process for Howard’s model such that survival of the cluster can be studied through coalescence of two neighbouring dual paths. It is important to observe that the dual process does not have the same distribution as time reversed forward process and we have limited understanding about the distribution of the dual process. Our proof uses the fact that under diffusive scaling, Howard’s model and it’s dual jointly converge in distribution to the Brownian web and it’s dual (Theorem 2.6 in [29]). Using joint convergence and non-crossing property of paths, we show that the coalescing time of the scaled paths also converge to the coalescing time of the limiting Brownian paths. This helps us in proving metric space convergence. In this sense the approach taken in this paper is much more robust.
We should mention here that Brownian web appears as universal scaling
limit for several discrete network models, e.g.,
discrete directed spanning forest model [28]
and collection of rightmost infinite open paths starting from all percolating points for supercritical oriented percolation [33]. For both these models, paths have complex interactions among themselves, but the same scaling limit should hold.
On the other hand it is important to remember that [22]
deals with ‘degenerate’ conditional set up {L(x,t)=n} and we are dealing with non-degenerate conditional set up {L(0,0)≥n}.
We would like to point out that
this work has at least one other motivation. It has been empirically observed that river networks are structurally self similar and satisfy various scaling laws. Study of these laws and understanding the reasons behind their existence are at the core of hydrology and for this, understanding the behaviour of the scaled tributaries are extremely important. Ferrarri et al. [26]predicted the same:
“The convergence results here may lead to
rigorous/alternative verification of some of the scaling theory for those (drainage) networks.”
Horton-Strahler ordering [15] is such an empirically observed scaling relation which represents scale invariance of a natural dendritic structure. Consider a binary rooted tree and assign order 1 to each leaf. The order of an internal vertex having children with orders i and j
respectively is given as
[TABLE]
Loosely speaking order of a branch denotes it’s relative importance in tree hierarchy.
Sequence of connected vertices of the same order is called branch.
While studying river streams, Horton [15] observed that
Nk+1/Nk≈R, 3≤R≤5.
This regularity has been strongly corroborated in hydrology ([31], [18], [37], [24])
and referred as Horton’s law.
The only rigorous result on validity of this law for drainage networks
was that of Shreve [32],
who demonstrated that for a uniform distribution of rooted binary trees
with n leaves, the ratio Nk+1/Nk converges to 4 as n→∞. To the best of our knowledge, there are only two other examples of binary random trees for which Horton self-similarity has been rigorously proved: the tree representation of a critical Galton
Watson binary branching process and tree representation of a Kingman’s coalescent process.
It is important to observe that for all these three models, there are no ‘space constraints’ as such.
In the context of drainage networks, any attempt to study Horton’s law requires a
complete understanding of the branching structure which has complex dependencies due to space constraint. Since T(0,0), the discrete tree obtained from the river delta C(0,0), contains all branching informations, it is hoped that finding this scaling limit may help in understanding Horton’s law. Note that, for Howard’s model T(0,0) is no longer a binary tree, but Horton-Strahler ordering can be extended for a general tree in a similar way.
This paper is organized as follows. In the next section we
construct the limiting CRT T
and explain the difference of T than the one described in [3]. In Section
3 we introduce the Brownian web and its dual and use them to prove that T is compact almost surely.
In Section 4 we describe a dual process for Howar’d model and prove Theorem 1.2. In the concluding section, i.e., Section 5 we make some remark about universality of our proof and present some further questions on properties of T.
2 Construction of the limiting CRT’s
In this section we construct the limiting CRT T.
We first observe that for (x,t)∈Z2, joining the successive
steps hk(x,t),hk+1(x,t):k≥0 by linear segments gives
a continuous path π(x,t) starting from x at time t and
moving in the forward direction of time as time is measured along the Y-axis. In other words
π(x,t)∈C[t,∞) is such that π(x,t)(t+k)=hk(x,t)(1)
for all k∈N∪{0}. Here and subsequently for (y,s)∈R2, π(y,s) denotes
an element in C[s,∞) with π(y,s)(s)=y. Graph distance between any two vertices in C(x,t) can be interpreted as sum of the times taken by the paths starting from each of the two vertices to coalesce.
In the following, we use this notion to obtain a tree-like metric space
from a given collection of paths satisfying certain conditions
(described below in Definition 2.2).
This notion will be used in the construction of T.
We start with a definition of tree-like metric space or real tree.
Definition 2.1**.**
A metric space (X,d) is called a real tree or a R-tree
if for all x,y∈X
(i)
there exists a unique geodesic from x to y, i.e., there exists a unique isometry fx,y:[0,d(x,y)]→X such that
fx,y(0)=x and fx,y(d(x,y))=y. The image of f(x,y) is denoted
by [[x,y]];
(ii)
the only non-self-intersecting path from x to y is
[[x,y]], i.e., if q:[0,1]→X is continuous and injective
such that q(0)=x and q(1)=y, then q([0,1])=[[xy]].
First condition says that X is a geodesic space, and the second is a tree property that there is a unique way to travel between any two points without backtracking.
Often it is assumed that a real tree is compact.
However for many purposes this assumption is not necessary and in
this paper we do not make such an assumption.
We mention here that the metric completion of an R-tree is also an R-tree (see [16]). Moreover it is known that the space of all isometry equivalence classes of compact real trees is closed
in M (Theorem 2.1 of [19]).
Next we describe a “tree-like” path space and how to obtain a real tree
out of it. Let Π be the collection of all continuous real valued paths
moving in the forward direction of time with all possible starting times
(for a formal definition see Subsection 3.1). In other words,
a path π∈Π with starting time σπ∈R
is a continuous mapping π:[σπ,∞)→R.
Similarly Π denotes the collection of all continuous real valued paths
moving in the backward direction of time with all possible starting times.
In what follows, paths moving in the forward
direction of time, will be referred to as forward paths and paths moving in the
backward direction of time, will be referred to as backward or dual paths.
The notation γ(π1,π2) defined as
γ(π1,π2):=inf{s>σπ1∨σπ2:π1(s)=π2(s)}
denotes the first intersection time of the
paths π1 and π2 strictly after time σπ1∨σπ2.
Definition 2.2** (Tree-like path space).**
K, a subset of Π, is said to be tree-like if the following conditions are satisfied:
(i)
γ(K):=sup{γ(π1,π2):π1,π2∈K}* is finite;*
(ii)
for all π1,π2∈K, we have (π1(σπ1),σπ1)=(π2(σπ2),σπ2) and π1(s)=π2(s) for all s≥γ(π1,π2).
These two conditions together imply that the paths in K coalesce
as soon as they intersect and hence they are non-crossing and all of them
coalesce in finite time.
The set {(π(s),s):π∈K,s∈[σπ,γ(K)]}
consists of the images of π in K upto time γ(K).
We assume that for any π∈K
and any t≥σπ, the path {π(s):s≥t} with starting time t is also in K.
We first observe that for a tree-like K⊂Π and for
any (y1,s1) in the image set, i.e., for (y1,s1)∈{(π(s),s):π∈K,s∈[σπ,γ(K)]},
there exists a unique path π(y1,s1) starting at (y1,s1) in K.
For any two points (y1,s1) and (y2,s2) in the image set, we define the ancestor metric dA((y1,s1),(y2,s2)) as,
[TABLE]
So, dA((y1,s1),(y2,s2))
adds the time taken by the two paths from their start till the time they meet.
With a slight abuse of notation, let M(K) denote the completion
of the metric space ({(π(s),s):π∈K,s∈[σπ,γ(K)]},dA). When γ(K) is finite, it is not difficult to see that this metric space is tree-like and
its completion M(K) is also an R-tree.
In exactly the same way,
this notion can be extended for a collection of tree-like
backward paths K⊂Π to obtain a complete R-tree
denoted by M(K).
We construct our limiting object now.
Consider two independent standard Brownian motions, B1,B2
with B1(0)=B2(0)=0. The random times τ1 and τ2 are defined as
[TABLE]
Both τ1 and τ2 are finite with τ2>τ1+1 a.s.
We define B+,B−∈C[0,∞] for t∈[0,τ2−τ1] as,
[TABLE]
For t>τ2−τ1 we take (B+,B−)(t):=(B1(τ1+t),B1(τ1+t)), i.e.,
the paths B+ and B− coalesce at time τ2−τ1.
Δ=Δ(B+,B−) denotes the region in R2
enclosed between the paths B+ and B−. Formally
[TABLE]
Now we consider countable family of coalescing backward (i.e., moving in the backward
direction of time) Brownian motions {Bm:m∈N}
starting from all rational vectors in Δ such that on hitting the forward paths B+ and
B−, they follow Skorohod reflection (see ). We explain this in more detail.
From the above family, consider a backward Brownian path Bm starting from
(xm,tm)∈Q2∩Δ. Consider another backward Brownian
path Bm′ starting from (xm,tm) independent of the forward paths B+ and B−.
Then the (joint) distribution of (B+,B−,Bm) is same as that of
(B+,B−,RB+,B−(Bm′)) where
RB+,B−(Bm′) is given as
[TABLE]
From the work of Soucialic et. al. it follows that the finite dimensional distributions
are consistent and hence {Bm:m∈N} exists.
By construction, we further have that the collection {Bm:m∈N}
gives a non-crossing coalescing path family with Bm(0)=0 for all m∈N.
We denote this collection of coalescing backward paths
as S=S(B+,B−):={Bm:m∈N}.
We observe that the collection
S satisfies the conditions of Definition
2.2 and gives a ‘tree-like path space’.
The limiting continuum random tree T is defined to be the complete metric space
M(S) where completion is taken w.r.t. the ancestor metric
for the tree like path space S.
Remark 2.3**.**
T** as conjectured in [3]:***
We remark here that a slightly different continuum random tree was surmised in [3]
as the scaling limit.
Since Aldous was interested about the scaling limit of the
discrete tree conditioned to have time-length exactly n, i.e.,
Tn(0,0)∣{L(0,0)=n},
the random region Δ was enclosed by two independent backward Brownian
motions both starting at the origin and conditioned to meet for the first time exactly at time −1. We are working with the “non-degenerate” conditioning {L(0,0)≥n}, hence in our case the region Δ=Δ(B+,B−) is enclosed by two independent backward Brownian motions both starting at the origin and conditioned to meet before time −1.
It is important to observe that for the continuum tree as described in [3], forward coalescing Brownian paths
coalesce with the boundary of Δ as soon as they hit the boundary
(see Page 276 of [3]). On the other hand, from the work of Soucaliuc et. al. [35], it follows that the forward coalescing Brownian paths follow Skorohod reflection
at the boundary of Δ(B+,B−).
This explains the difference of the limiting T from the predicted one in [3].*
3 Double Brownian web and compactness of T, T
In this section, we prove that T is compact almost surely.
Towards this we introduce a related random object,
called the double Brownian web, i.e., the Brownian web and its dual, denoted by (W,W) and show that
a version of S(B+,B−) can be embedded in (W,W).
This allows us to use properties of (W,W) to prove compactness. The proof of Theorem 1.2 also uses properties of (W,W).
3.1 Brownian web and its dual
The Brownian web originated in the work of Arratia (see [1]).
Later Fontes et. al. [11] studied the Brownian web as a random variable taking values in an appropriate Polish space. We recall the relevant details from [11].
Let Rc2 denote the completion of the space time plane R2 with
respect to the metric
[TABLE]
As a topological space Rc2 can be identified with the
continuous image of [−∞,∞]2 under a map that identifies the line
[−∞,∞]×{∞} with the point (∗,∞), and the line
[−∞,∞]×{−∞} with the point (∗,−∞).
A path π in Rc2 with starting time σπ∈[−∞,∞]
is a mapping π:[σπ,∞]→[−∞,∞]∪{∗} such that
π(∞)=∗ and, when σπ=−∞, π(−∞)=∗.
Also t↦(π(t),t) is a continuous
map from [σπ,∞] to (Rc2,ρ).
We then define Π to be the space of all paths in Rc2 with all possible starting times in [−∞,∞].
The following metric, for π1,π2∈Π
[TABLE]
makes Π a complete, separable metric space. The metric dΠ is slightly different
from the original choice in [11] which is somewhat less natural as explained
in [36].
Remark 3.1**.**
Convergence in the (Π,dΠ) metric can be described as locally uniform convergence of paths as well as convergence of starting times. Therefore, for any ϵ>0
and m>0,
we can choose ϵ1(=g(ϵ,m))>0 such that for π1,π2∈Π with {(πi(t),t):t∈[σπi,m]}⊆[−m,m]×[−m,m] for i=1,2 and dΠ(π1,π2)<ϵ1 imply that
∣σπ1−σπ2∣∨∣π1(σπ1)−π2(σπ2)∣<ϵ and sup{∣π1(t)−π2(t)∣:t∈[σπ1∨σπ2,m]}<ϵ.
∎
Let H denote the space of compact subsets of (Π,dΠ) equipped with the Hausdorff metric dH.
As (Π,dΠ) is Polish, it follows that (H,dH)
is also Polish. Let
BH be the Borel σ−algebra on the metric space (H,dH).
The Brownian web W is an (H,BH) valued random variable characterized as (Theorem 2.1 of [11]):
Theorem 3.2**.**
There exists an (H,BH) valued random variable
W such that whose distribution is uniquely determined by
the following properties:
(a)
for each deterministic point z∈R2
there is a unique path πz∈W starting from z almost surely;
(b)
for a finite set of deterministic points z1,…,zk∈R2,
the collection (πz1,…,πzk) is distributed as coalescing Brownian motions starting from z1,…,zk;
(c)
for any countable deterministic dense set D⊂R2,
W is the closure of {πz:z∈D} in (Π,dΠ) almost surely.
The above theorem shows that the collection is
almost surely determined by countably many coalescing Brownian motions.
The metric space of compact sets of backward paths is defined similarly and denoted
by (H,dH). Let
BH be the corresponding Borel σ field.
(W,W) is a (H×H,BH×H) valued random variable such that W and W uniquely determine each other
with W being equally distributed as −W,
the Brownian web rotated 1800 about the origin. Theorem 5.8 of [10] and
Theorem 2.4 of [34] give characterizations of
the double Brownian web (W,W).
Before ending this subsection we list some properties of
(W,W) which hold almost surely
and which will be used later.
The type of a point (x,t) is given by (min(x,t),mout(x,t)).
Similarly we define min(x,t) and mout(x,t)
for the dual paths.
It is known that (see Proposition 5.12, Theorem 5.13 and Theorem 5.16 of [10])
(i)
min(x,t)+1=mout(x,t) and
mout(x,t)−1=min(x,t).
(ii)
Every deterministic point (x,t)∈R2 is of type (0,1).
(iii)
For any deterministic time t, the type of any point on R×{t} is one of (0,1),(0,2) and (1,1) in W.
(b)
Let D⊆R2 be a deterministic countable dense set.
For any (x,t)∈D, there exists a unique path π(x,t)∈W
distributed as a Brownian motion starting from (x,t).
(c)
Paths in W meet and coalesce when they meet, i.e., for each π,π′∈W we have γ(π,π′)<∞ and π(s)=π′(s) for all s≥γ(π,π′) (see Proposition 3.2 of [34]).
(d)
For every π∈W and π∈W
(i)
there does not exist any s,t∈[σπ,σπ] with (π(s)−π(s))(π(t)−π(t))<0, i.e., no forward path of W crosses a dual path of W;
(ii)
∫σπσπ1{π(s)=π(s)}ds=0, i.e.,
forward paths of W and dual paths of W “spend zero Lebesgue time together”
(see Proposition 3.2 in [36]).
(e)
For any t>0,t0∈R
(i)
the set {π(t0+t):π∈W,σπ≤t0} is locally finite (see Proposition 4.3 in [11]);
(ii)
for any x∈{π(t0+t):π∈W,σπ≤t0}, there exist π1,π2∈W both starting from
the point (x,t0+t) such that π2(s)=π1(s) for all s∈[t0,t0+t) (follows from (a));
(iii)
for any x∈{π(t0+t):π∈W,σπ≤t0}, there exist π1,π2∈W with σπ1<t0<σπ2 such that π1(t0+t)=π2(t0+t)=x (follows from (d) (ii), (b) and (c)).
(f)
For each point (x,t)∈R2 and any two sequences {xn−:n≥1},{xn+:n≥1}⊂
such that xn−↑x and xn+↓x, consider the paths π(xn−,t),π(xn+,t)∈W, starting from (xn−,t),(xn+,t) respectively. The limits limn→∞π(xn−,t) and limn→∞π(xn+,t) exist
and do not depend on the choice of the sequences {xn−:n≥1},{xn+:n≥1}
(see Proposition 3.2 (e) of [36]).
(g)
For {πn:n≥1}⊆W and π~∈W
with dΠ(πn,π~)→0, we have that γ(πn,π~)→σπ~ as n→∞
(see Lemma 3.4 of [36]).
3.2 Compactness of T
We first show that a version of S(B+,B−) can be embedded
in W. We need to introduce some notations.
Let π(0,0)∈W denote the forward Brownian path in W
starting from the origin. For ease of notation we take π0=π(0,0).
Let θ0≤0 be defined as,
[TABLE]
In other words, the point (π0(θ0),θ0)
has 2 outgoing dual paths and π1 is the ‘newly born’
path in W, which starts at (π0(θ0),θ0)
and do not coalesce with π0 within the time (θ0,θ0+1).
θ1 denotes the coalescing time of these two paths,
and we have θ1>θ0+1 a.s.
Define
[TABLE]
S(π0,π1) precisely represents the collection of dual paths
in W starting from all rational vectors
in the region enclosed between π0 and π1.
From property (c) of (W,W), it follows that
S(π0,π1) satisfies the conditions of Definition 2.2.
We consider the complete metric space {\cal M}\bigl{(}\widehat{{\cal S}}(\pi_{0},\pi_{1})\bigr{)} with the ancestor metric and show that it has the same distribution as T.
Proposition 3.3**.**
We have
[TABLE]
Assuming the above proposition we first prove that T is compact almost surely.
Proposition 3.4**.**
T* is compact almost surely.*
Proof :
Because of Proposition 3.3, it suffices to show that
the metric space, {\cal M}\bigl{(}{\cal S}(\widehat{\pi}_{0},\widehat{\pi}_{1})\bigr{)} is compact almost surely.
Being complete, it is enough to show that it is totally bounded as well. Fix ϵ>0 and set δ=δ(ω)∈(0,((θ0−θ1)−1∧ϵ)/4).
For j≥1, let tjδ:=θ1+jδ and jmax:=min{j≥1:tj+1δ>θ0}.
Because of property (e) of (W,W), for any 1≤j≤jmax−1
the set
{π(tj+1δ):σπ≤tjδ,π∈S(π0,π1)} is finite. Since M(S(π0,π1)) is the completion of \bigl{(}\{(\pi(s),s):\pi\in{\cal S}(\widehat{\pi}_{0},\widehat{\pi}_{1}),s\in[\sigma_{\pi},\theta_{0}]\},d_{{\cal A}}\bigr{)}, the choice of δ ensures that the collection
[TABLE]
forms a finite ϵ-cover for {\cal M}\bigl{(}{\cal S}(\widehat{\pi}_{0},\widehat{\pi}_{1})\bigr{)}.
This completes the proof.
∎
Now we proceed to prove Proposition 3.3.
We need to introduce some notations.
We define π+,π−∈C[0,∞] as
[TABLE]
Since the dual paths in W starting from all rational points distributed as
coalescing backward Brownian motions and follow Skorohod reflection at the forward
paths in W, in order to prove Proposition 3.3,
it suffices to show that, as elements in C[0,∞)×C[0,∞)
To prove Proposition 3.3 we need to deal with two issues. First of all,
the random time θ0 is not a stopping time. Secondly, the properties of
(W,W) readily gives us that for each (x,t)∈Q2, there exists
unique path in W distributed as Brownian motion starting from (x,t).
The point (π0(θ0),θ0) is random and to obtain the distribution of
(π−,π+), we have to approximate them using skeletal Brownian paths
starting from rational points.
Let B0 and B1/n denote coalescing Brownian motions starting from the points
(0,0) and (1/n,0) respectively. Let γn:=γ(B0,B1/n)
denote the coalescing time of these two paths.
The following proposition is the main tool for proving Proposition 3.3,
which shows that as n→∞, the conditional distribution of (B1/n,B0)∣{γn≥1} converges to (B+,B−). We believe that Proposition 3.5 could be of independent interest.
Proposition 3.5**.**
As n→∞, we have
[TABLE]
In order to prove the conditional limit theorem, we need to introduce some notations.
Following the construction of (B+,B−), for general
f1,f2∈C[0,∞) with f1(0)=f2(0)=0, we define
[TABLE]
For n≥1 we define
[TABLE]
Let A,An⊂C[0,∞)×C[0,∞) be such that
[TABLE]
Consider the mapping Γ:C[0,∞)×C[0,∞)→C[0,∞)×C[0,∞)
where Γ(f1,f2):=(f1,f2) for (f1,f2)∈/A.
For (f1,f2)∈A with f1(λ0)=f2(λ0)=y0∈R, we
define
[TABLE]
Similarly for n≥1, the mapping Γn:C(−∞,0]×C(−∞,0]→C(−∞,0]×C(−∞,0] is defined as Γn(f1,f2):=(f1,f2) for (f1,f2)∈/An.
For (f1,f2)∈An with f1(λ0n)=f2(λ0n)=y0n, we define
[TABLE]
Before we proceed further, we state the following deterministic
corollary which will be used
in the proof of Proposition 3.3. For the time being,
we postpone the proof of Corollary 3.6.
Corollary 3.6**.**
For (f1,f2)∈C(−∞,0]×C(−∞,0] with λ1(f1,f2)<λ0(f1,f2)−1, we have
[TABLE]
under the product metric.
Now we are ready to prove Proposition 3.5
and its proof is motivated from Lemma 3.1 of [7].
Proof of Proposition 3.5:
Let B1,B2 are two independent Brownian motions starting from
the origin. We observe that almost surely,
as pair of paths (B1,B2)∈An for all n≥1.
We first show that for all n≥1, we have
[TABLE]
For t>0 and n≥1, we define the event Etn as
[TABLE]
We note that occurrence of the event Etn implies that there exists some s0<t
such that ∣(B1−B2)(s0)∣=1/n with ∣(B1−B2)(s′)∣>0
for all s′∈(s0,t∧(s+1)).
By definition we have that for all t>0, the event Etn is
Ft:=σ({B1(s),B2(s):0≤s≤t}) measurable.
For any t>0 and for n≥1 we have
[TABLE]
as non-occurrence of the event Etn ensures that the random time λ0n can not occur earlier than t and the event {∣B1(s1)−B2(s1)∣>0 for all s1∈[t,t+1]}∩{∣B1(t)−B2(t)∣=1/n} confirms it can not occur later than t.
Set B1(λ0n)∧B2(λ0n)=y0n.
Using B1,B2 now we define B1′,B2′∈C[0,∞) as
[TABLE]
For any Borel set B⊆C[0,∞)×C[0,∞), we obtain
[TABLE]
The event (Etn) is measurable w.r.t. the σ-field
Ft:=σ({B1(s),B2(s):0≤s≤t})
and from Markov property of (B1,B2)
it follows that given {∣(B1−B2)(t)∣=1/n,∣(B1−B2)(s1)∣>0 for all s1∈[t,t+1],(Etn)c}, the distribution of the
process {(B1′(t+s),B2′(t+s)):s≥0} does not depend on Etn and
has the same distribution as two independent coalescing
Brownian motions starting from the points (1/n,0) and (0,0) respectively and conditioned
not to meet before time 1. Hence from (3.2), we obtain
Now fix any bounded continuous function f:C[0,∞)×C[0,∞)↦R.
[TABLE]
Since f is chosen arbitrarily, this completes the proof.
∎
Now we use Proposition 3.5 to prove Proposition 3.3.
Proof of Proposition 3.3:
As observed earlier it suffices to prove (8).
Recall that π0 is the dual path in W starting from the point (0,0). For n≥1 let ln and rn be rationals given by ln:=(⌊nπ0(θ0)⌋)/n and
rn:=ln+1/n where θ0 is as defined as in (6).
We choose θ0n∈(θ0−1/n,θ0)∩Q such that
(i)
π0(s),π1(s)∈[ln,rn) for all s∈[θ0n,θ0] where π1 is the dual path in W starting from (π0(θ0),θ0),
(ii)
θ0n>θ1+1.
Since θ0>θ1+1 almost surely and both the backward continuous paths π0 and π1 pass through the point (π0(θ0),θ0), such θ0n always exists. Clearly θ0n→θ0 as n→∞.
For all n≥1 both (ln,θ0n) and (rn,θ0n) are in Q2 and
let π(ln,θ0n) and π(rn,θ0n) denote the dual
paths in W starting from the points (ln,θ0n) and (rn,θ0n)
respectively. Since the dual paths in W are non-crossing, condition (ii) implies that π(rn,θ0n)(θ0n−1)>π(ln,θ0n)(θ0n−1). The backward paths πn+,πn−∈C(−∞,0] are defined as
[TABLE]
By construction we have πn+(0)−πn−(0)=1/n and
πn+(s)>πn−(s)
for all s∈[−1,0] almost surely.
Since W is compact, both the sequences {π(rn,θ0n):n∈N}
and {π(ln,θ0n):n∈N} must have convergent subsequences.
As convergence of paths implies convergence of starting times as well, subsequential limits of each of these two sequences must be backward paths in W
starting at (π0(θ0),θ0).
From the properties of (W,W) we have that there are exactly two dual paths starting from the point (π0(θ0),θ0). Hence it follows that
[TABLE]
where the limit is taken in (Π,dΠ).
This shows that the sequences of
dual paths, {πn+:n∈N} and {πn−:n∈N},
almost surely converge to the dual paths π+ and π− respectively.
Fix any bounded continuous function g:C(−∞,0]×C(−∞,0]↦R.
We claim that
[TABLE]
The proof is similar to the proof of Lemma LABEL:lem:ConditionalStoppingTime.
For completeness we present here full details.
For each n≥1, let On denote the event that the set of the points {π0(θ0−1),π1(θ0−1)} equals the set {π(ln,θ0n)(θ0−1),π(rn,θ0n)(θ0−1)}.
From (14) and from property (g) of (W,W), we have that
P(On)→1 as n→∞.
Hence we have
[TABLE]
where 1On denotes indicator function of the event On.
We need to define some more events.
For t>0 and n≥1, let Ft denote the event that
[TABLE]
As W is compact, the sequence of dual paths {πm′:m∈N} considered in the event Ft must have a subsequential limit.
Hence occurrence of the event Ft ensures existence of a dual path π1∈W starting from (π0(−s0),−s0) for some s0<t such that
π0((−s0−1)∨(−t))=π1((−s0−1)∨(−t)).
Next for t>0,i∈Z and s∈Q, we define the following events :
[TABLE]
where π(ni+1,s) and π(ni,s) are the dual paths in W starting from the points (ni+1,s) and (ni,s) respectively.
For t>0 with a slight abuse of notation let Gt denote the σ-field given by
[TABLE]
By definition for all t>0, both the events Ft and Et(i,n) are
Gt measurable.
Hence from non-crossing nature of paths in W it follows that for all t>0 and for t0n∈(t,t+1/n)∩Q, we have the following equality of events
[TABLE]
For t>0 and for t0n∈(t,t+1/n)∩Q using (16) and (3.2) we obtain
[TABLE]
Next we observe that conditioned on the event that (Ft)c∩Et(i,n,−t0n)∩{π0(s),π1(s)∈[i/n,(i+1)/n) for all s∈[−t0n,−t]}, the process {(π(ni+1,−t0n)(−t0n−s)−i/n,π(ni,−t0n)(−t0n−s)−i/n):s≥0} is independent of the σ-field Gt0n and has the same distribution as (W(1/n,0),W(0,0))∣{γn<−1}. Since {π0(s),π1(s)∈[i/n,(i+1)/n) for all s∈[−t0n,−t]}∩(Ft)c
is Gt0n measurable, from (3.2) we obtain
[TABLE]
This completes the proof of (15).
Since (πn+,πn−)→(π+,π−) almost surely as n→∞, from Lemma 4.4 and Corollary 3.6 we have
[TABLE]
This completes the proof.
∎
Finally we need to complete the proof of Corollary 3.6.
Proof of Corollary 3.6: We observe that for all large n, both λ1n(f1,f2) and λ0n(f1,f2) are finite and λ1n(f1,f2)<λ0n(f1,f2)−1. Fix ϵ>0. For ease of notations, we take λ0=λ0(f1,f2),λ1=λ1(f1,f2),λ0n=λ0n(f1,f2) and λ1n=λ1n(f1,f2). Since f1,f2 are both continuous with f1(0)=f2(0)=0, we have λ0n≤λ0 and λ1n≤λ1 for all large n. Set n0 such that λ0n≤λ0,λ1n=λ1 and 1/n<ϵ/2 for all n≥n0. Choose δ>0 such that
the following conditions hold :
(i)
min{∣f1(s)−f2(s)∣:s∈[λ0−1−δ,λ0−δ]}=β>0,
(ii)
sup{∣f1(x)−f1(y)∣∨∣f2(x)−f2(y)∣:x,y∈[λ1,0],∣x−y∣<δ}<ϵ/2 and
(iii)
sup{∣f1(x)−f2(y)∣:x,y∈[λ1−δ,λ1+δ]}<ϵ/2.
Since f1 and f2 are both continuous with f1(λ1)=f2(λ1) and λ1 is strictly smaller than λ0−1, δ>0 always exists.
Condition (ii) ensures that λ0n≥λ0−
Because of condition (i), for all n>1/β we have
λ1n∈(λ0−δ,λ0) and consequently λ1n=λ1. Further the conditions (ii) and (iii) mentioned above imply that
[TABLE]
Since ϵ>0 is chosen
arbitrarily, (3.2) completes the proof.
∎
The embedding discussed in Proposition 3.3 proves the following corollary:
Corollary 3.7**.**
For any ϵ∈(0,1) and for π1,π2∈S(B+,B−) with σπ1∨σπ2≤−ϵ, almost surely there exists s0=s0(ω)∈(−ϵ,0) such that π1(s)=π2(s) for all s≥s0.
Proof : The proof follows from Proposition 3.3
and from property (a) of (W,W) which ensures that min(π0(θ0),θ0)=1 almost surely.
∎
The same argument as in Proposition 3.3 gives us the following
corollary:
Corollary 3.8**.**
We end this section with the following two remarks:
Remark 3.9**.**
Conditional that the point (x,t) is a (1,2) type point, i.e., one incoming path and two outgoing
paths (see Section 3 for a detailed definition) such that these two outgoing paths,
denoted by π+(x,t) and π−(x,t), don’t coalesce before time t+1.
We define (π+,π−)∈C[0,∞)×C[0,∞) such that
[TABLE]
Same argument as in Proposition 3.3 gives us the distributional equality
[TABLE]
Remark 3.10**.**
Regarding the construction of T, it is useful to mention
here that instead of taking closure with respect to the ancestor metric,
one can take closure of S(B+,B−) in (Π,dΠ).
The embedding explained in Proposition 3.3
shows that in that case the resulting collection of dual paths will no longer satisfy
the condition of Definition 2.2,
as almost surely there will be (random) points with
multiple outgoing paths. Nevertheless, the resulting object almost surely will be an
R-graph (for a formal definition and basic properties of an R-graph, see [8]).
For constructing the limiting real tree, one could have also followed
cutting operation of this R-graph as in [8].
Finally we comment that the distribution of (T,T)
does not depend on the choice of the deterministic countable dense set of R2.
In this section we prove Theorem 1.2.
Before embarking on the details, we sketch the idea of the proof.
Coletti et. al. [25] showed that the scaled Howard’s model
observed as collection of paths, converges in distribution to the Brownian web
(see Theorem in [25]). Later, Roy et. al. constructed a dual
network for the Howard’s model and showed that under diffusive scaling, Howard’s
model and it’s dual jointly converges in distribution to the Brownian web and it’s
dual (Theorem of [29]). We use this joint convergence in path-space topology
and prove that a scaled pair of Howard paths together with it’s coalescing time
(which is finite due to due to Theorem 1.1) jointly
converges in distribution to a pair of coalescing Brownian paths and their coalescing time.
This enables us to obtain convergence of metric spaces in the Gromov-Hausdorff topology.
We need to introduce some notation.
For (x,t)∈Z2, taking the edges
⟨hk−1(x,t),hk(x,t)⟩
to be straight line segments for k≥1, we parametrize the path formed by these edges as
the piece wise linear function π(x,t):[t,∞)→R
such that π(x,t)(t+k)=hk(x,t)(1) for every integer k≥0 and
and linear in between.
Let X:={π(x,t):(x,t)∈Zeven2} denote the collection of all (forward) paths obtained from G.
For each n≥1 and for π∈Π, the scaled path
πn:[σπ/n,∞]→[−∞,∞] is given by πn(t):=π(nt)/n.
For each n≥1, let Xn:={πn(x,t):(x,t)∈Zeven2} be the collection of the scaled paths and
Xˉn is the closure of
Xn in (Π,dΠ).
As we commented earlier, in order to obtain the scaling limit one has to deal
with the complex dependencies between multiple paths. Coletti et. al. showed that
under diffusive scaline, the Howard’s model converges in distribution to the
Brownian web.
As n→∞, Xˉn
converges in distribution to the Brownian web W as
H,BH) valued random variables.
Later Roy et. al. constructed a dual graph for Howard’s model
and extended the above result to obtain joint convergence to the double Brownian web
(W,W) for Howard’s model and it’s dual under diffusive scaling.
Similarly we construct a scaled family of backward/dual paths obtained from G.
We need to explain the dual graph first.
For (x,t)∈Zodd2,
the dual path π(x,t) is the piecewise linear function π(x,t):(−∞,t]→R
with π(x,t)(t−k)=hk(x,t)(1) for every integer k≥0.
Let X:={π(x,t):(x,t)∈Zodd2}
be the collection of all possible dual paths admitted by G.
For the backward path π, the scaled version is
πn:[−∞,σπ/n]→[−∞,∞] given by πn(t)=π(nt)/n for each n≥1.
Let Xn:={πn(x,t):(x,t)∈Zodd2} be the collection of all the n th order diffusively scaled dual paths.
The following theorem regarding the joint
convergence of (Xˉn,Xn) to (W,W) is due to Roy * et. al.* [29].
As n→∞, (Xˉn,Xn)
converges in distribution to the double Brownian web (W,W) as (H×H,BH×H) valued random variables.
We will use Theorem 4.2
to prove Theorem 1.2. First we introduce
some notation. For t∈R and K⊆Π, let Kt−:={π∈K:σπ≤t} denote the collection of paths in K which start before time t.
Similarly for K⊆Π, let Kt+:={π∈K:σπ≥t} denote the collection of dual paths in K which start after time t.
Let ξK⊂R be defined as
[TABLE]
For x∈ξK, for K⊂Π and K⊂Π,
let πr(x,0)=πr(x,0)(K×K) be defined to be the path π∈K with σπ=0 and such that there is no other path
π′∈K0+ with x<π′(0)<π(0); if no such
π∈K exists then we define πr(x,0) to be the backward constant zero function o starting at σo=0.
In other words πr(x,0) is the path of K0+ which intersects the x-axis to the right of (x,0) and is the closest such path to do so.
Similarly we define πl(x,0) as the path of K0+ which intersects the x-axis to the left of (x,0) and is the closest such path to do so. Let γ(l,r):=γ(πr(x,0),πl(x,0)) be the first meeting time of the two backward paths πl(x,0) and
πr(x,0) (which can possibly be −∞).
Let Δ=Δr,l(x)⊂R2 denote the region enclosed between these two backward paths, πl(x,0) and πr(x,0), and formally defined as
[TABLE]
If γ(l,r) is finite then this region is also bounded .
Let D:={(x/n,t/n):(x,t)∈Zeven2,n∈N}
and
[TABLE]
the closures being taken in (Π,dΠ) and (Π,dΠ) respectively.
We further assume that (K,K) is such that,
for each x∈ξK both the collections, S(πr(x,0),πl(x,0)) and S(πr(x,0),πl(x,0)), are tree-like in the sense of Definition 2.2 and by construction both S(πr(x,0),πl(x,0)) and S(πr(x,0),πl(x,0)) are families of coalescing paths.
The completions of these spaces with respect to the ancestor metric are defined as
[TABLE]
We further assume that for each x∈ξK, both these metric spaces, M(x,0) and M(x,0), are compact
and let ϕ(M(x,0)) and ϕ′(M(x,0))
denote the isometric embeddings of the metric spaces M(x,0) and M(x,0) into M respectively, the metric space of isometric equivalence classes of compact
metric spaces endowed with the Gromov-Hausdorff metric.
Fix f:M×M→R, a bounded continuous real valued function and define
[TABLE]
For the rest of the section we make two specific choices of (K,K), namely, (W,W) and (Xn,Xn). Also to simplify notation we write
[TABLE]
It is known that E(η)=1/π.
As observed in [RSS15],
for each x∈ξ, there exist two dual paths
πr(x,0),πl(x,0)∈W
both starting at (x,0) such that πr(x,0)(−1)>πl(x,0)(−1) with γ(r,l) finite. Hence the region Δr,l(x)(W,W) is almost surely non-empty and bounded.
From the properties of (W,W) we have that both the path spaces, S(πr(x,0),πl(x,0))(W×W) and
S(πr(x,0),πl(x,0))(W×W), are tree-like in the sense of Definition
2.2.
Same argument as in Proposition 3.4 shows
that both the metric spaces, M(W,W)(x,0)
and M(W,W)(x,0), are compact as well. Similarly
for n≥1 and for each xn∈ξn, the region
Δr,l(x)(Xn,Xn) is almost surely nonempty and bounded.
From the construction it follows that, both the families, S(πr(xn,0),πl(xn,0))(Xn,Xn) and S(πr(xn,0),πl(xn,0))(Xn,Xn), satisfy the condition
of Definition 2.2 and both these metric spaces, M(Xn,Xn)(xn,0) and M(Xn,Xn)(xn,0), are compact.
Hence the random variables κ(f):=κ(W,W)(f), and κn(f):=κ(Xn,Xn)(f) are well defined almost surely.
In the next subsection we calculate E(κ(f)).
4.1 Calculation of E(κ(f))
The aim of this subsection is to prove the following proposition which calculates E(κ(f)).
Proposition 4.3**.**
We have
E(κ(f))=E(f(ϕ(T),ϕ′(T)))/π.
To prove this proposition we need to prove a limit result
for conditional continuum random trees. Recall that
W(0,0) and W(1/n,0), are two independent coalescing backward Brownian motions starting from the
points (0,0) and (1/n,0) respectively with their coalescing time γn=γ(W(1/n,0),W(0,0)).
Let Δ(W(0,0),W(1/n,0))
denote the random region enclosed between these two backward Brownian paths, defined as
[TABLE]
We construct an equivalent of (T,T) here.
We start coalescing backward Brownian motions
from all points of Δ(W(1/n,0),W(0,0))∩Q2
such that these backwards paths coalesce with the boundary of
Δ(W(1/n,0),W(0,0)) as soon as they intersect
the boundary. This collection of coalescing backward paths is denoted by S(W(1/n,0),W(0,0)).
From earlier discussions it follows that for each (x,t)∈Δ(W(1/n,0),W(0,0))∩Q2, there exists a forward path π(x,t)∈Π which does not cross any dual path in S(W(1/n,0),W(0,0)) and defined as
[TABLE]
We denote this collection of forward paths starting from all the points of Δ(W(1/n,0),W(0,0))∩Q2 by S(W(1/n,0),W(0,0)). Because of property (d) of (W,W), the set {π(0):π∈S(W(1/n,0),W(0,0)), σπ≤−1} is almost surely finite.
Let xn=xn(ω)∈(0,1/n) be defined as
[TABLE]
Next we consider all the paths in S(W(1/n,0),W(0,0))
which pass through xn. In other words we consider a new collection of coalescing paths S′(W(1/n,0),W(0,0)) defined as S′(W(1/n,0),W(0,0)):={π∈S(W(1/n,0),W(0,0)):π(0)=xn}.
By construction, both S′(W(1/n,0),W(0,0)) and S(W(1/n,0),W(0,0))
are tree-like in the sense of Definition 2.2.
For n≥1 we consider the pair of complete metric spaces
[TABLE]
Similar argument as in the proof of Proposition 3.4
shows that these metric spaces are also compact almost surely. It is useful to observe that for each n≥1, the metric space Tn does not depend on how the forward paths evolve after time
[math].
Lemma 4.4**.**
[TABLE]
where convergence in distribution holds with respect to the Gromov-Hausdorff topology.
Assuming the above lemma we first calculate E(κ(f)) and complete the proof
of Proposition 4.3.
Proof of Proposition 4.3 :
Let In⊂{0,1,…,n−1} be given by
[TABLE]
For i∈In, let
Δ(π((i+1)/n,0),π(i/n,0))
denote the random region enclosed by the two backward Brownian paths π((i+1)/n,0) and π(i/n,0) and let
[TABLE]
For i∈In, let xin=xin(ω)∈(i/n,(i+1)/n) be defined as
[TABLE]
We recall that for each i∈In, the set {π(0):π∈W(−1)−,π(0)∈(i/n,(i+1)/n)} is nonempty and finite and hence xin is well defined.
Next we define the coalescing family of forward paths passing through xin given as
[TABLE]
From the properties of (W,W) it follows that both these collections of
paths, S′(π((i+1)/n,0),π(i/n,0)) and
S(π((i+1)/n,0),π(i/n,0)), are tree-like
and we consider the complete metric spaces
[TABLE]
For i∈In, the paths in S′(π((i+1)/n,0),π(i/n,0))
do not cross the dual paths in S(π((i+1)/n,0),π(i/n,0)) and (π((i+1)/n,0),π(i/n,0)) is
distributed as coalescing backward Brownian motions starting from ((i+1)/n,0) and (i/n,0) conditioned to meet after time −1. Hence for each i∈In we have
[TABLE]
Fix a bounded continuous function g:M×M→R.
We define
[TABLE]
where ϕi/n and ϕi/n′ are isometric embeddings of the respective metric spaces into M, the space of all isometry equivalence classes of compact metric spaces.
We want to show that
[TABLE]
where ϕx,ϕx′ are the corresponding embeddings of the respective metric spaces into M.
We first show that #In→#ξ=η as n→∞. Choose n0=n0(ω)
such that for all x,y∈ξ and for n≥n0 we have ∣x−y∣>2/n.
For each x∈ξ, set lnx=⌊nx⌋/n
and rnx=lnx+(1/n).
From the non-crossing nature of paths in W it follows that for each x∈ξ, we have
π(rnx,0)(−1)>π(lnx,0)(−1) and hence lnx∈In.
Hence #In≥ξ for all n≥n0.
On the other hand for each i∈In, choose yi such that
yi∈(π(i/n,0)(−1),π((i+1)/n,0)(−1))∩Q and consider the path π(yi,−1) in W. Then we must have
π(yi,−1)(0)=xi∈ξ. This implies that
#In≤#ξ for all n.
Hence for all n≥n0 we have #In=#ξ.
This ensures that for all large n,
[TABLE]
Choose n1=n1(ω)≥n0 large enough such that
for all n≥n1 we have #In=η and consequently for all n≥n1 and for each x∈ξ we have
[TABLE]
We recall that there are exactly two dual paths πr(x,0) and πl(x,0) starting from (x,0) with πr(x,0)(−1)>πl(x,0)(−1). Hence
from property (f) of (W,W) it follows that,
{π(lnx,0):n∈N} and {π(rnx,0):n∈N}
converge to πl(x,0) and πr(x,0) respectively
in (Π,dΠ) as n→∞.
Let γ(πl(x,0),π(lnx,0)) denote the coalescing time of the two dual paths
π(lnx,0) and πl(x,0).
Similarly the coalescing time of the two dual paths
π(rnx,0) and πr(x,0) is given by
γ(πr(x,0),π(rnx,0)).
For all n≥n0 and for each x∈ξ, the metric space M(W,W)(x,0) is naturally embedded into M(S(π(rnx,0),π(lnx,0))). Using this embedding we obtain that for all n≥n1 and for each x∈ξ we have
[TABLE]
Now because of property (g) of (W,W), we have that (γ(πl(x,0),π(lnx,0)),γ(πr(x,0),π(rnx,0)))→(0,0) as n→∞.
Since g is continuous on the product metric space and the set ξ is finite, (25), (26) and (27) show that
[TABLE]
As g is bounded and E[η]<∞, the family {Rn(g):n∈N} is uniformly integrable and hence we have
[TABLE]
From (24) and for B∈[0,∞) denoting a standard Brownian motion we have,
[TABLE]
where Φ is the distribution function of a standard normal random variable.
The last step follows from Lemma 4.4.
This completes the proof.
∎
Proof of Lemma 4.4 :
Recall that B1 and B2 are two independent
backward Brownian motions both starting from the origin. We observe that (B1,B2)∈An almost surely for all n≥1.
The proof of Corollary 3.6 shows that
(λ1n,λ0n)→(λ1,λ0) as n→∞ almost surely.
Choose n0=n0(ω) so that for all n≥n0 we have
λ0n∈(λ1,λ0) and consequently λ1n=λ1.
For all n≥n0, the set {π(λ0n−λ0):π∈S(B+,B−),σπ≤(λ0n−λ0)−1} is nonempty and finite.
We take yn∈R as yn:=min{π(λ0n−λ0):π∈S(B+,B−),σπ≤(λ0n−λ0)−1}.
Next we consider the coalescing families of forward and backward paths defined by
[TABLE]
Let M(Sn(B+,B−)) and M(Sn(B+,B−)) denote the corresponding complete metric spaces
where completions are taken with respect to the ancestor metric.
We observe that both these metric spaces are naturally embedded into the metric spaces
M(S(B+,B−))=T and M(S(B+,B−))=T respectively.
We show that almost surely
[TABLE]
as n→∞. Fix ϵ>0 and choose n1=n1(ω)≥n0 such that (λ0−λ0n)<ϵ/2 for all n≥n1.
We first observe that the natural embedding shows that
dGH(M(Sn(B+,B−)),T)≤2(λ0−λ0n)<ϵ for all n≥n1.
In order to get an upper bound for dGH(M(Sn(B+,B−)),T), from Remark 3.10 we obtain that for all π1,π2∈S(B+,B−) with σπ1∨σπ2≤−ϵ/2
there exists s0=s0(ω)∈(0,ϵ/2) which does not depend on the choice of π1,π2 such that for all s≥−s0 we have π1(s)=π2(s). Choose n2=n2(ω)≥n1
such that 1/n2<s0.
Then for any π∈S(B+,B−) with σπ≤−ϵ/2 we have π∈Sn(B+,B−) as well for all n≥n2. Hence we have dGH(M(Sn(B+,B−)),T)≤ϵ for all n≥n2. This proves (28).
Finally same argument as in Lemma LABEL:lem:ConditionalStoppingTime shows that
(Tn,Tn)∣{γn<−1} converges in distibution to (T,T) as n→∞.
∎
4.2 Convergence of E(κn(f))
In this subsection we prove that
E(κn(f))→E(κ(f)) as n→∞
and use it to prove Theorem 1.2. In order to prove the above mentioned convergence, we first need to show that E(ηn)→E(η) as n→∞.
For t1<t2 let
[TABLE]
Below we prove a continuity property of η(s,0):s<0, which will be used in proving convergence of E(ηn).
Corollary 4.5**.**
We have lims↓−1η(s,0)=η a.s.
Proof :
For −1≤s1≤s2<0 we have ξ(s1,0)⊆ξ(s2,0) and consequently η(s1,0)≤η(s2,0). Because of this monotonicity lims↓−1η(s,0)
exists almost surely. Since ξ⊆ξ(s,0) for all s∈(−1,0),
we have ξ⊆⋂s∈(−1,0)ξ(s,0), implying that
lims↓−1η(s,0)≥η.
If lims↓−1η(s,0)>η, then there exists x∈ξ(−1/2,0)∖ξ and
a sequence of paths {πn∈W} with πn(0)=x for all n
such that −1<σπn≤−1/2 and
σπn decreases to −1 as n→∞.
By compactness of W,
it follows that there exists a convergent subsequence {πnk:k∈N}
and π∈W such that
πnk→π in (Π,dΠ) as k→∞. Since convergence in (Π,dΠ) implies convergence of starting times also, we must have
σπ=−1 and π(0)=x which
contradicts the choice of x and the proof follows.
∎
Next we use Corollary 4.5 to prove convergence of E(ηn).
Lemma 4.6**.**
E[ηn]→E[η]* as n→∞.*
Proof :
We show that ηn converges in distribution
to η as n→∞ and the sequence
{ηn:n∈N} is uniformly integrable as well.
Recall from Theorem [11] that
(Xˉn,Xˉn)⇒(W,W) as n→∞.
Using Skorohod’s representation theorem
we assume that we are working on a probability space such that
[TABLE]
almost surely as n→∞. Same argument as in Lemma 3.2 of [RSS15]
shows that ηn converges to η almost surely as n→∞. For completeness we present the proof here also.
First we show that, for all k≥0,
[TABLE]
Indeed, for k=0, both 1{ηn≥k} and 1{η≥k} equal 1. We need to show (29) for k≥1.
From Properties of (W,W) it follows that
η is finite and ξ⊂(0,1) almost surely. Hence
we can choose 0<ϵ=ϵ(ω) such that
(i)
for all x,y∈ξ with x=y we have (x−ϵ,x+ϵ)⊂(0,1) and ∣x−y∣>2ϵ;
(ii)
for all x∈ξ there exists π∈W with
σπ≤−1−ϵ and π(0)=x.
Let m=m(ω)>0 be such that
[TABLE]
Choose n0=n0(ω) such that for all n≥n0,
dH×H((W,W),(Xˉn,Xˉn))<g(ϵ,m) where g(ϵ,m)
is as in Remark 3.1.
By the choice of n0, it follows that for each π∈W(−1−ϵ)−
with π(0)∈[0,1] and for all n≥n0, there
exists πn∈Xn with σπn≤−1 and dΠ(π,πn)<g(ϵ,m). Since ∣π(0)−πn(0)∣<ϵ,
from the choice of ϵ we must have πn(0)∈(0,1). Thus ηn(ω)≥k for all n≥n0.
This proves (29).
Finally we need to show that
P(limsupn→∞{ηn>η})=0.
This is equivalent to showing that P(Ω0k)=0 for all k≥0,
where
[TABLE]
Consider k=0 first. Using Corollary 4.5
we can obtain l0:=l0(ω)∈(−1,0)
such that η(l0,0)(ω)=η(ω).
Since both the points (0,0) and (1,0) are of type (0,1) and
on the event {η=0}
the set ξ(l0,0)=ξ=∅,
we can obtain ϵ:=ϵ(ω)∈(0,1+l0)
such that for all π∈W(ω)
with σπ≤−1+ϵ≤l0, π(0)∈/(−ϵ,1+ϵ).
On the event Ω00, choose large enough n such that ηn(ω)>0 and
dH×H((W,W),(Xˉn,Xˉn))<g(ϵ,m) where m=m(ω)>0 is chosen as in
(30) and g(ϵ,m) is as in Remark 3.1.
From the choice of ϵ, it follows that there exists π∈W(ω)
with σπ≤−1+ϵ and π(0)∈(−ϵ,1+ϵ). This
gives a contradiction. Hence we have P(Ω00)=0.
For k>0, on the event Ω0k we show that
a forward path π∈W coincides with a dual path π∈W for a positive time which leads to a contradiction.
From Corollary 4.5 it follows that,
we can choose −1<l0(ω)<−1/2 such that ξ(l0,0)(ω)=ξ(ω).
From property (a) of (W,W) it further follows that
for any x∈ξ, the type of the point (x,0) is (1,1).
Hence for each x∈ξ there exists sx=sx(ω)∈(−1,0) such that for any π1,π2∈Wl0− with
π1(0)=π2(0)=x, we have π1(s)=π2(s) for all s≥sx.
Set s0:=max{sx:x∈ξ} and observe that s0<0 almost surely.
By definition, for all s≥s0 we have #{π(s0):π∈Wl0−,π(1)∈[0,1]}=k. This gives us that ξ(l0,0)(ω)=ξ(ω)=ξ(l0,s0)(ω), i.e., the paths leading to any single point considered in ξ(l0,0)
have coalesced before time s0. We consider k paths contributing to ξ(l0,0), viz., π1,…,πk
such that {π1(0),…,πk(0)}=ξ(l0,0). Choose 0<ϵ=ϵ(ω)<min{∣s0∣,1+l0}/3 such that
(i)
(x−ϵ,x+ϵ)⊂(0,1) for all x∈ξ(l0,0);
(ii)
the ϵ-tubes around π1,…,πk, given by
[TABLE]
are disjoint.
Choose m=m(ω)>0 as in (30).
Set n0=n0(ω) such that for all n≥n0, ξn0(ω)>k
and
[TABLE]
where g(ϵ,m)
is as in Remark 3.1.
By the choice of n0, it follows that one of the k tubes must contain at least two paths, π1n0,π2n0 (say)
of Xn0(−1)− which do not coalesce by time [math].
From the construction of dual paths it follows that there exist at least one dual
path πn0∈Xn0
lying between π1n0 and π2n0 for t∈[−1,0] and hence
we must have an approximating π∈W close to
πn0 for t∈[−1,−ϵ]. More formally there exists a dual path π∈W(−ϵ)+ such that supt∈[−1,−ϵ]∣π(t)−πn0(t)∣<ϵ and thus supt∈[s0,−ϵ]∣π(t)−π(t)∣<4ϵ.
Now select any sequence ϵl↓0 with ϵl<ϵ for
all l≥1. By the above procedure we can select πl∈W with σπl≥−ϵl>−ϵ
such that supt∈[s0,−ϵ]∣πl(t)−π(t)∣<4ϵl for some π∈{π1,…,πk}. Since we have only finitely many paths π1,…,πk, we can choose πi for some 1≤i≤k and a subsequence πlj so that supt∈[s0,−ϵ]∣πlj(t)−πi(t)∣<4ϵlj for all j≥1.
By the compactness of W,
there exists π∈W with σπ≥−ϵ such that π(t)=πi(t) for t∈[s0,−ϵ].
This violates property (e) of Brownian web and its dual listed earlier.
Hence P(Ω0k)=0 for all k≥0 and this completes the proof that
ηn→η almost surely as n→∞.
Now it suffices to show that the sequence {ηn:n∈N} is uniformly integrable. As ηn→η almost surely, using Proposition 4.1 of [11]
for any k≥1 we have,
[TABLE]
We have used the fact that P(η≥1) is same as the probability that two independent Brownian motions starting at unit distance do not meet by time 1, which is strictly smaller
than 1. This completes the proof.
∎
Remark 4.7**.**
It is important to observe that the argument for uniform integrability presented
here depends only on the fact that ηn→η almost surely whereas the argument of Lemma 3.3 of [RSS15] uses some model specific assumptions.
We comment here that similar arguments show
that ηn(t0,t1)→η(t0,t1) almost surely for any t0<t1.
We first prove Theorem 1.2 assuming Lemma 4.8 holds.
Proof of Theorem 1.2:
Recall that for (x,t)∈Zeven2 and for π(x,t)∈X, i.e.,
the path in X starting from (x,t), the n -th order diffusively scaled path
is denoted by πn(x,t). For (x,t)∈Zeven2 and for n≥1, let
[TABLE]
Both the path spaces, Sn(x,t) and Sn(x,t), are tree-like in the sense of
Definition 2.2 and we consider the complete metric spaces
M(Sn(x,t)) and M(Sn(x,t)).
It follows that for all (x,t)∈Zeven2 and for all n≥1, we have
that both the metric spaces Tn(x,t) and Tn(x,t) are naturally embedded into
the metric spaces M(Sn(x,t)) and M(Sn(x,t)) respectively.
This embedding ensures that for all n≥1 we have
[TABLE]
Hence to prove Theorem 1.2 it suffices to show that
[TABLE]
Using translation invariance of our model, we have
Since f is chosen arbitrarily, this completes the proof.∎
We now prove Lemma 4.8.
Since f is bounded, uniform integrability of {κn(f)} follows from uniform integrability of {ηn:n∈N}.
Hence to prove Lemma 4.8,
it suffices to show that κn(f)→κ(f) almost surely as n→∞.
We introduce some notation now.
On the event {η=1}, Lemma 4.6 ensures that there exists n0=n0(ω) such that ηn=1 for all n≥n0.
For n≥n0 consider x=x(ω),xn=xn(ω)∈R
such that ξ={x} and ξn={xn}.
For ease of notation on the event {η=1} and for n≥n0 we take
[TABLE]
In what follows, we assume that we are working on
a probability space such that (Xˉn,Xˉn) converges
to (W,W) almost surely in (H×H,dH×H).
Lemma 4.9**.**
On the event {η=1}, we have
dH×H((Sn,Sn),(S,S))→0
almost surely as n→∞.
Proof :
We prove that dH(Sn,S)→0 as n→∞
almost surely. The argument for dH(Sn,S) is exactly the same and hence omitted.
Fix ϵ>0.
Choose δ=δ(ω)∈(0,ϵ)∩Q
such that
[TABLE]
Assume that ξ(−δ,0)={x,x1,…,xk} where ξ={x}.
We choose γδ=γδ(ω)∈(0,ϵ)
such that (a) the points in ξ(−δ,0) are at least 2γδ distance apart, i.e., ∣x−xi∣∧∣xi−xj∣>2γδ for all 1≤i<j≤k and (b) (x−γδ,x+γδ) as well as (xi−γδ,xi+γδ) are both included in the interval (0,1) for all 1≤i≤k.
We mentioned earlier that there exist
dual paths πr(x,0),πl(x,0) in W
both starting at (x,0) such that
πr(x,0)(−1)>πl(x,0)(−1). Similarly for each xi∈ξ(−δ,0) there exist dual paths πr(xi,0),πl(xi,0) in W both starting at (xi,0) such that
πr(xi,0)(−δ)>πl(xi,0)(−δ)
for all 1≤i≤k. Because of continuity, there exists νδ=νδ(ω)>0 such that πr(x,0)(−1−νδ)>πl(x,0)(−1−νδ) and πr(xi,0)(−δ−νδ)>πl(xi,0)(−δ−νδ) for 1≤i≤k.
From properties (f) and (g) of (W,W) (see Subsection 3.1) it follows that there exist πl,πr,πli,πri∈W such that all these dual paths have starting times strictly
larger than [math] and
[TABLE]
This gives that
[TABLE]
From Remark 4.7 we have {\mathbb{P}}\bigl{(}\bigcap_{t\in[-1,0)\cap{\mathbb{Q}}}\{\lim_{n\to\infty}\eta_{n}(t,0)=\eta(t,0)\}\bigr{)}=1.
Set ζδ>0 such that
[TABLE]
Let n1=n1(ω)>max{4/νδ,1/δ,n0} be such that,
for all n≥n1
(i)
ηn(−δ,0)=η(−δ,0) and ηn=η;
(ii)
dH×H((W,W),(Xˉn,Xˉn))<g(min{γδ,ζδ,ϵ}/4,m) where m is defined as in (30) and the value g(min{γδ,ζδ,ϵ}/4,m) is taken as in Remark 3.1.
The choice of n1 and ζδ ensure that
there exist πrn,πln∈Xn0+, and
for all 1≤i≤k there exist
πi,rn,πi,ln∈Xn0+ such that
[TABLE]
as well as
πrn(−1)>πln(−1) and
πi,rn(−δ−νδ)>πi,ln(−δ−νδ) for all 1≤i≤k.
Therefore, there exists a forward path ϑn∈Xn(−1)− such that πln(−1)<ϑn(−1)<πrn(−1). Using (31) we further have that x−γδ<πln(0)<ϑn(0)<πrn(0)<x+γδ.
Similarly for each 1≤i≤k there exists a forward path ϑin∈Xn(−δ)− such that (a) πi,ln(−δ)<ϑin(−δ)<πi,rn(−δ)
and (b) xi−γδ<πi,ln(0)<ϑin(0)<πi,rn(0)<xi+γδ.
Since for all n≥n1 we have #ξn(−δ,0)=k+1,
hence ξn(−δ,0)={ϑin(0):1≤i≤k}∪{ϑn(0)}. Thus,
[TABLE]
We observe that (yn,0)=(nϑn(0),0) is in Zeven2
and the vertices (yn+1,0),(yn−1,0) are the right and left dual neighbours of
(yn,0) respectively. Similarly (yin,0)=(nϑin(0),0)∈Zeven2 for 1≤i≤k.
For any πn∈Sn we have πn(0)=xn and hence for all n≥n1, using (32) and (33) obtain
[TABLE]
For any π1,π2∈S and π1n,π2n∈Sn we have
π1(s)=π2(s) and π1n(s)=π2n(s) for all s≥0 with ∣π1n(0)−π1(0)∣<ϵ. This observation together with the fact that sups1,s2∈[(−2δ)∨σπ1,0]{∣π1(s1)−π1(s2)∣}≤sups1,s2∈[−2δ,0]{∣πr(s1)−πl(s2)∣}<ϵ ensures that
to prove Lemma 4.9, it suffices to show that
[TABLE]
Fix π∈S with σπ≤−2δ.
From the choice of n1 it follows that for all n≥n1 there exists an
approximating path πn∈Xn(−δ)− with ∣π(0)−πn(0)∣<γδ. As σπn≤−δ, we have πn(0)∈ξ(−δ,0).
Since π∈S, it
follows that π(0)=x. Hence from the uniqueness as mentioned in (4.2), it follows that for all n≥n1 the approximating path πn must have
πn(0)=xn implying that πn∈Sn.
Similar argument shows that for all n≥n1 and for πn∈Sn with σπn≤−δ, there exists approximating path in S.
This completes the proof.
∎
Before stating the next lemma we give an alternate definition of dGH which will be used in our proof. For two compact metric spaces (X1,d1) and (X2,d2), a correspondence between
X1 and X2 is a subset R of X1×X2 such that for every x1∈X1 there exists at least one x2∈X2 such that (x1,x2)∈R and conversely for every y2∈X2
there exists at least one y1∈X1 such that (y1,y2)∈R. The distortion of a correspondence R is defined by
[TABLE]
Then, if X1 and X2 are two real trees, we have
[TABLE]
where C(X1,X2) denotes the set of all correspondences between X1 and X2.
Using Lemma 4.9 we prove the
following lemma which is the main lemma of this section.
Lemma 4.10**.**
On the event {η=1} we have
dGH(ϕn(Mn),ϕ(M))∨dGH(ϕn′(Mn),ϕ′(M))→0
almost surely as n→∞, where ϕn,ϕ,ϕn′,ϕ′ denote the corresponding embeddings of the respective metric spaces into M.
Proof : Before proving this lemma we first sketch the key idea.
The metric dH×H deals with the path space topology, convergence in this metric does not ensure that the coalescing times also converge (even if they are finite). Using joint convergence of the collection of forward paths together with the collection of dual paths, we
show that the coalescing times of the scaled paths converge jointly to the coalescing time of the limiting Brownian paths and this gives convergence with respect to the ancestor metric. We first show that dGH(ϕn(Mn),ϕ(M))→0 as n→∞ almost surely and the argument for
dGH(ϕn′(Mn),ϕ′(M))→0 as n→∞ is exactly the same.
Using Definition (35), it suffices to show that
there exists a correspondence Rn between
Mn and M such that
[TABLE]
Choose any sequence {ϵk:k∈N} such that
ϵk↓0 as k→∞. For k≥1, let nk=nk(ω)∈N be such that dH(Snk,S)<g(ϵk/8,m) almost surely where
m is defined as in (30) and g(ϵ,m) as in Remark 3.1.
We define correspondences Rn for large n only.
For nk≤n<nk+1, we define our correspondence Rn between Mn
and M as
[TABLE]
For all nk≤n<nk+1, (4.2) gives a valid correspondence.
Aiming for a contradiction suppose (36) does not hold.
As dΠ(π1,π2)<g(ϵk/8,m) implies that
∣σπ1−σπ2∣<ϵk/8,
if (36) does not hold then there exists
β=β(ω)>0 such that
[TABLE]
where for ease of notation we take γ(1,2)k=γ(π1k,π2k) and γ(1,2)n=γ(π1n,π2n).
Choose k0 such that ϵk∨(1/nk)<β/8 for all k≥k0.
From (4.2), it follows that there are infinitely many k≥k0 such that there exist π1k,π2k∈S and π1n,π2n∈Sn for some nk≤n<nk+1 with dΠ(π1k,π1n)∨dΠ(π2k,π2n)<g(ϵk/8,m) and ∣γ(1,2)k−γ(1,2)n∣>β/2.
We consider the two cases :
(a)
γ(1,2)n>γ(1,2)k+β and
(b)
γ(1,2)n≤γ(1,2)k−β.
For (a) from the choice of k0, it follows that for infinitely many k≥k0
and for some nk≤n<nk+1
we have σπ1n∨σπ2n≤γ(1,2)k+β/4
with π1n(γ(1,2)k+β)=π2n(γ(1,2)k+β).
From the construction of the dual graph it follows that for infinitely many k≥k0
and for some nk≤n<nk+1,
there exists πn∈Sn with σπn≥γ(1,2)k+3β/4 and for s∈[γ(1,2)k,γ(1,2)k+3β/4] we have πn(s)∈(π1n(s)∧π2n(s),π1n(s)∨π2n(s)).
Hence we have
∣πn(s)−π1k(s)∣<ϵk/2 for all
s∈[γ(1,2)k,γ(1,2)k+3β/4].
Since dH×H((Sn,Sn),(S,S))<g(ϵk/8,m) for all n≥nk,
for infinitely many k≥k0 there exists πk∈S with σπk≥γ(1,2)k+β/4
and dΠ(πk,πnk)<ϵk/8.
This gives us that ∣πk(s)−π1k(s)∣<ϵk for all
s∈[γ(1,2)k,γ(1,2)k+β/4].
For (b) we need a slightly different argument.
From the properties of (W,W) discussed earlier, it follows that there exists
πk∈S starting from the point (π1k(γ(1,2)k),γ(1,2)k) and lying between the forward paths π1k and π2k in the time interval [σπ1k∨σπ2k,γ(1,2)k].
For s∈[γ(1,2)k−β/4,γ(1,2)k] we have
π1n(s)=π2n(s). Since
dΠ(πik,πin)<g(ϵk/8,m) for i=1,2,
it follows that 0<∣π1k(s)−π2k(s)∣<ϵk/4 for all
s∈[γ(1,2)k−β/4,γ(1,2)k].
Since the dual path πk starting from the point (π1k(γ(1,2)k),γ(1,2)k) lies between π1k and π2k, we have that
∣πk(s)−π1k(s)∣<ϵk/4 for all
s∈[γ(1,2)k−β/4,γ(1,2)k].
Since ϵk↓0, because of compactness of (W,W),
this contradicts the fact that in the double Brownian web almost surely no two
forward path and dual path spend positive Lebesgue measure time together.
This completes the proof.
∎
Finally we prove Lemma 4.8 to complete the proof of Theorem
1.2.
Proof of Lemma 4.8 :
Since f is bounded, the uniform integrability of the sequence {κn(f);n∈N}
follows from that of the sequence {ηn:n∈N}.
Since ηn→η almost surely, κn(f)→κ(f) holds trivially on the event {η=0}.
On the event {η=1}, using continuity of f this follows from
Lemma 4.10). For general k≥1 on the event {η=k}, the proof is similar.
∎
5 Concluding remark
To the best of our knowledge
both these continuum random trees, T and T, have not been studied
in the literature so far. On the other hand, the system of coalescing Brownian motions starting from every space-time points on R2 has been
extensively studied but with respect to a different topology (see
[11], [34] for details).
It should be mentioned here that coalescing Brownian motions starting from all the points in R
at a given time has been studied as a genealogical tree in [27] with respect
to a different topology where the spatial locations of the points are also taken care of.
Further understanding of these continuum random trees T and T
might be useful and we present some questions towards that direction.
In the above construction we have used the fact that the collection of
forward paths S(B+,B−) in the region Δ(B+,B−) is almost surely uniquely determined by the
collection of backward or dual paths S(B+,B−).
It should be possible to construct T
directly as completion of the metric space obtained from the system of
coalescing forward Brownian paths starting from all the points of
Δ(B+,B−)∩Q2,
which follow Skorohod reflection at the boundary
of Δ(B+,B−). In order to do that construction, one
has to show that starting from finitely many space-time points such a collection satisfies
Kolmogorov’s consistency conditions, as it does not directly follow from [35].
From the construction of (T,T), it is reasonable to expect that T almost surely determines T and vice-versa. One possible to way to prove this is to show that
the contour function of T is determined by T and vice-versa and in that case T can be regarded as the dual tree of T.
It is natural to ask how are the contour functions of these two continuum random trees distributed? Presently we do not have any understanding about these processes.
Finally in the context of drainage network scaling relations, it might be of interest to
see whether these two continuum trees obey Horton’s law or not.
Acknowledgements:
The author thanks Siva Athreya, Manjunath Krishnapur, Rahul Roy, Rongfeng Sun and Sreekar Vadlamani for discussion and comments. Part of the work was done when the author was a visiting scientist at Indian Statistical Institute, Bangalore center.
Bibliography37
The reference list from the paper itself. Each links out to its DOI / PubMed record.
1[1] Arratia, R. (1979). Coalescing Brownian motions on the line. Ph.D. dissertation, Univ. Wisconsin, Madison.
2[2] Aldous, D. (1991) The continuum random tree I. Ann. Probab. 19 1-28.
3[3] Aldous, D. (1993) The continuum random tree III. Ann. Probab. 21 248-289.
4[4] Aldous, D. (1997) Brownian excursions, critical random graphs and the multiplicative coalescent. Ann. Probab. 25 812-854.
5[5] Berry, L. Ã., Broutin, N. and Goldschmidt, C. (2012) The continuum limit of critical random graphs. Probab. Theory Related Fields 152 367-406.
6[6] Aldous, D. and Pittel, B. (2000) On a random graph with immigrating vertices: Emergence of the giant component. Random Structures Algorithms 17 79-102.
7[7] Bolthausen, E. (1976) On a functional central limit theorem for random walks conditioned to stay positive. Ann. Probab. 4 480-485.
8[8] Berry, L. Ã., Broutin, N., Goldschmidt, C. and Miermont, G. (2015) The scaling limit of the minimum spanning tree of a complete graph. ar Xiv:1301.1664