Stable maps: scaling limits of random planar maps with large faces - - PowerPoint PPT Presentation

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Stable maps: scaling limits of random planar maps with large faces - - PowerPoint PPT Presentation

Stable maps: scaling limits of random planar maps with large faces G. Miermont , joint with J.-F . Le Gall Dpartement de Mathmatiques dOrsay Universit de Paris-Sud Conformal maps from probability to physics Ascona, 24 May 2010 G.


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SLIDE 1

Stable maps: scaling limits of random planar maps with large faces

  • G. Miermont, joint with J.-F

. Le Gall

Département de Mathématiques d’Orsay Université de Paris-Sud

Conformal maps from probability to physics Ascona, 24 May 2010

  • G. Miermont (Orsay)

Random maps with large faces CMPP Ascona 1 / 24

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SLIDE 2

Planar maps

Definition

A planar map is a proper embedding of a connected graph in the two-dimensional sphere, considered up to direct homeomorphisms of the sphere. A rooted map: an oriented edge (e) is distinguished A pointed map: a vertex (v∗) is distinguished Notations:

◮ V(m) set of vertices ◮ F(m) set of faces ◮ dgr the graph distance

  • G. Miermont (Orsay)

Random maps with large faces CMPP Ascona 2 / 24

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SLIDE 3

Planar maps

Definition

A planar map is a proper embedding of a connected graph in the two-dimensional sphere, considered up to direct homeomorphisms of the sphere. A rooted map: an oriented edge (e) is distinguished A pointed map: a vertex (v∗) is distinguished Notations:

◮ V(m) set of vertices ◮ F(m) set of faces ◮ dgr the graph distance

  • G. Miermont (Orsay)

Random maps with large faces CMPP Ascona 2 / 24

slide-4
SLIDE 4

Planar maps

Definition

A planar map is a proper embedding of a connected graph in the two-dimensional sphere, considered up to direct homeomorphisms of the sphere. A rooted map: an oriented edge (e) is distinguished A pointed map: a vertex (v∗) is distinguished Notations:

◮ V(m) set of vertices ◮ F(m) set of faces ◮ dgr the graph distance

  • G. Miermont (Orsay)

Random maps with large faces CMPP Ascona 2 / 24

slide-5
SLIDE 5

Planar maps

Definition

A planar map is a proper embedding of a connected graph in the two-dimensional sphere, considered up to direct homeomorphisms of the sphere. A rooted map: an oriented edge (e) is distinguished A pointed map: a vertex (v∗) is distinguished Notations:

◮ V(m) set of vertices ◮ F(m) set of faces ◮ dgr the graph distance

  • G. Miermont (Orsay)

Random maps with large faces CMPP Ascona 2 / 24

slide-6
SLIDE 6

Planar maps

Definition

A planar map is a proper embedding of a connected graph in the two-dimensional sphere, considered up to direct homeomorphisms of the sphere.

e v∗

A rooted map: an oriented edge (e) is distinguished A pointed map: a vertex (v∗) is distinguished Notations:

◮ V(m) set of vertices ◮ F(m) set of faces ◮ dgr the graph distance

  • G. Miermont (Orsay)

Random maps with large faces CMPP Ascona 2 / 24

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SLIDE 7

Natural ways of picking a map at random

All maps we consider are rooted. pick a p-angulation with n vertices, uniformly at random (ex p = 3 triangulation, p = 4 quadrangulation) From now on we only consider bipartite plane maps (with faces of even degree) Boltzmann distribution: let q = (qk, k ≥ 1) a non-negative

  • sequence. Define a measure on the set of (rooted) planar maps by

Wq(m) =

  • f∈F(m)

qdeg(f)/2 . Let Pq(·) = Wq(·) Zq , where Zq =

m Wq(m) is finite iff there exists x > 1 such that

  • k≥0

xk 2k + 1 k

  • qk+1 = 1 − 1

x .

  • G. Miermont (Orsay)

Random maps with large faces CMPP Ascona 3 / 24

slide-8
SLIDE 8

Natural ways of picking a map at random

All maps we consider are rooted. pick a p-angulation with n vertices, uniformly at random (ex p = 3 triangulation, p = 4 quadrangulation) From now on we only consider bipartite plane maps (with faces of even degree) Boltzmann distribution: let q = (qk, k ≥ 1) a non-negative

  • sequence. Define a measure on the set of (rooted) planar maps by

Wq(m) =

  • f∈F(m)

qdeg(f)/2 . Let Pq(·) = Wq(·) Zq , where Zq =

m Wq(m) is finite iff there exists x > 1 such that

  • k≥0

xk 2k + 1 k

  • qk+1 = 1 − 1

x .

  • G. Miermont (Orsay)

Random maps with large faces CMPP Ascona 3 / 24

slide-9
SLIDE 9

Natural ways of picking a map at random

All maps we consider are rooted. pick a p-angulation with n vertices, uniformly at random (ex p = 3 triangulation, p = 4 quadrangulation) From now on we only consider bipartite plane maps (with faces of even degree) Boltzmann distribution: let q = (qk, k ≥ 1) a non-negative

  • sequence. Define a measure on the set of (rooted) planar maps by

Wq(m) =

  • f∈F(m)

qdeg(f)/2 . Let Pq(·) = Wq(·) Zq , where Zq =

m Wq(m) is finite iff there exists x > 1 such that

  • k≥0

xk 2k + 1 k

  • qk+1 = 1 − 1

x .

  • G. Miermont (Orsay)

Random maps with large faces CMPP Ascona 3 / 24

slide-10
SLIDE 10

Natural ways of picking a map at random

All maps we consider are rooted. pick a p-angulation with n vertices, uniformly at random (ex p = 3 triangulation, p = 4 quadrangulation) From now on we only consider bipartite plane maps (with faces of even degree) Boltzmann distribution: let q = (qk, k ≥ 1) a non-negative

  • sequence. Define a measure on the set of (rooted) planar maps by

Wq(m) =

  • f∈F(m)

qdeg(f)/2 . Let Pq(·) = Wq(·) Zq , where Zq =

m Wq(m) is finite iff there exists x > 1 such that

  • k≥0

xk 2k + 1 k

  • qk+1 = 1 − 1

x .

  • G. Miermont (Orsay)

Random maps with large faces CMPP Ascona 3 / 24

slide-11
SLIDE 11

Natural ways of picking a map at random

All maps we consider are rooted. pick a p-angulation with n vertices, uniformly at random (ex p = 3 triangulation, p = 4 quadrangulation) From now on we only consider bipartite plane maps (with faces of even degree) Boltzmann distribution: let q = (qk, k ≥ 1) a non-negative

  • sequence. Define a measure on the set of (rooted) planar maps by

Wq(m) =

  • f∈F(m)

qdeg(f)/2 . Let Pq(·) = Wq(·) Zq , where Zq =

m Wq(m) is finite iff there exists x > 1 such that

  • k≥0

xk 2k + 1 k

  • qk+1 = 1 − 1

x .

  • G. Miermont (Orsay)

Random maps with large faces CMPP Ascona 3 / 24

slide-12
SLIDE 12

Boltzmann distributions (continued)

Under Pq, it holds that the degrees of the faces of m form an independent, identically distributed family of random variables, when these faces are explored in an appropriate way to be explained later. The common law is that of a typical face f ∗, e.g. the face incident to the root edge of the map. Let W n

q (·)

= Wq

  • ·
  • {m has n vertices}
  • =

Pq(· | {m has n vertices}) , defining a probability measure. The conditions on q for writing W n in the second form are more stringent: note that by Euler’s formula V − E + F = 2 W n

q = W n q′

if q′

k = βk−1qk,

W n is uniform on 2p-angulations with n vertices if qk = δkp.

  • G. Miermont (Orsay)

Random maps with large faces CMPP Ascona 4 / 24

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SLIDE 13

Boltzmann distributions (continued)

Under Pq, it holds that the degrees of the faces of m form an independent, identically distributed family of random variables, when these faces are explored in an appropriate way to be explained later. The common law is that of a typical face f ∗, e.g. the face incident to the root edge of the map. Let W n

q (·)

= Wq

  • ·
  • {m has n vertices}
  • =

Pq(· | {m has n vertices}) , defining a probability measure. The conditions on q for writing W n in the second form are more stringent: note that by Euler’s formula V − E + F = 2 W n

q = W n q′

if q′

k = βk−1qk,

W n is uniform on 2p-angulations with n vertices if qk = δkp.

  • G. Miermont (Orsay)

Random maps with large faces CMPP Ascona 4 / 24

slide-14
SLIDE 14

Boltzmann distributions (continued)

Under Pq, it holds that the degrees of the faces of m form an independent, identically distributed family of random variables, when these faces are explored in an appropriate way to be explained later. The common law is that of a typical face f ∗, e.g. the face incident to the root edge of the map. Let W n

q (·)

= Wq

  • ·
  • {m has n vertices}
  • =

Pq(· | {m has n vertices}) , defining a probability measure. The conditions on q for writing W n in the second form are more stringent: note that by Euler’s formula V − E + F = 2 W n

q = W n q′

if q′

k = βk−1qk,

W n is uniform on 2p-angulations with n vertices if qk = δkp.

  • G. Miermont (Orsay)

Random maps with large faces CMPP Ascona 4 / 24

slide-15
SLIDE 15

Boltzmann distributions (continued)

Under Pq, it holds that the degrees of the faces of m form an independent, identically distributed family of random variables, when these faces are explored in an appropriate way to be explained later. The common law is that of a typical face f ∗, e.g. the face incident to the root edge of the map. Let W n

q (·)

= Wq

  • ·
  • {m has n vertices}
  • =

Pq(· | {m has n vertices}) , defining a probability measure. The conditions on q for writing W n in the second form are more stringent: note that by Euler’s formula V − E + F = 2 W n

q = W n q′

if q′

k = βk−1qk,

W n is uniform on 2p-angulations with n vertices if qk = δkp.

  • G. Miermont (Orsay)

Random maps with large faces CMPP Ascona 4 / 24

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SLIDE 16

Scaling limits of random 2p-angulations

Let Mn be a uniform 2p-angulation with n vertices. Endow the set V(Mn) of its vertices with the usual graph distance dgr. Then ([Chassaing-Schaeffer], for p = 2) it holds that typical distances are of order n1/4 as n → ∞. More generally, one expects a convergence of the form (V(Mn), n−1/4dgr) − →

n→∞ (S, cpd) ,

(1) for some constant cp > 0, where (S, d) is a random metric space, the Brownian map.

Theorem (Le Gall, Le Gall-Paulin)

For every increasing sequence in N, there exists a sub-sequence along which the convergence (1) holds in distribution for the Gromov-Hausdorff topology on compact metric spaces. The limit (S, d) is a.s. homeomorphic to S2, and has Hausdorff dimension a.s. dimH(S, d) = 4 .

  • G. Miermont (Orsay)

Random maps with large faces CMPP Ascona 5 / 24

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SLIDE 17

Scaling limits of random 2p-angulations

Let Mn be a uniform 2p-angulation with n vertices. Endow the set V(Mn) of its vertices with the usual graph distance dgr. Then ([Chassaing-Schaeffer], for p = 2) it holds that typical distances are of order n1/4 as n → ∞. More generally, one expects a convergence of the form (V(Mn), n−1/4dgr) − →

n→∞ (S, cpd) ,

(1) for some constant cp > 0, where (S, d) is a random metric space, the Brownian map.

Theorem (Le Gall, Le Gall-Paulin)

For every increasing sequence in N, there exists a sub-sequence along which the convergence (1) holds in distribution for the Gromov-Hausdorff topology on compact metric spaces. The limit (S, d) is a.s. homeomorphic to S2, and has Hausdorff dimension a.s. dimH(S, d) = 4 .

  • G. Miermont (Orsay)

Random maps with large faces CMPP Ascona 5 / 24

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SLIDE 18

Scaling limits of random 2p-angulations

Let Mn be a uniform 2p-angulation with n vertices. Endow the set V(Mn) of its vertices with the usual graph distance dgr. Then ([Chassaing-Schaeffer], for p = 2) it holds that typical distances are of order n1/4 as n → ∞. More generally, one expects a convergence of the form (V(Mn), n−1/4dgr) − →

n→∞ (S, cpd) ,

(1) for some constant cp > 0, where (S, d) is a random metric space, the Brownian map.

Theorem (Le Gall, Le Gall-Paulin)

For every increasing sequence in N, there exists a sub-sequence along which the convergence (1) holds in distribution for the Gromov-Hausdorff topology on compact metric spaces. The limit (S, d) is a.s. homeomorphic to S2, and has Hausdorff dimension a.s. dimH(S, d) = 4 .

  • G. Miermont (Orsay)

Random maps with large faces CMPP Ascona 5 / 24

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SLIDE 19

Scaling limits for Boltzmann-distributed maps

When q is ‘regular enough’ (e.g. decreasing sufficiently fast), then degrees of typical faces of a W n

q -sampled map are exponentially

  • tight. Intuitively, faces remain small:

◮ the maximal degree is of order log n, ◮ distances are still of the order n1/4. ◮ One expects the scaling limit to be still the Brownian map

[Marckert-M.,M.-Weill].

But if for some a ∈ (3/2, 5/2), we have q◦

k ∼ k−a ,

k → ∞ and qk = cβkq◦

k for the appropriate “critical” value of (c, β), then

the typical face in a Pq-sampled map has heavy tail Pq(deg f ∗ ≥ k) ∼ Cqk−α , k → ∞ where α = a − 1/2 ∈ (0, 2). Consequently, the largest face of a W n

q -disributed map has degree

  • f order n1/α.
  • G. Miermont (Orsay)

Random maps with large faces CMPP Ascona 6 / 24

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SLIDE 20

Scaling limits for Boltzmann-distributed maps

When q is ‘regular enough’ (e.g. decreasing sufficiently fast), then degrees of typical faces of a W n

q -sampled map are exponentially

  • tight. Intuitively, faces remain small:

◮ the maximal degree is of order log n, ◮ distances are still of the order n1/4. ◮ One expects the scaling limit to be still the Brownian map

[Marckert-M.,M.-Weill].

But if for some a ∈ (3/2, 5/2), we have q◦

k ∼ k−a ,

k → ∞ and qk = cβkq◦

k for the appropriate “critical” value of (c, β), then

the typical face in a Pq-sampled map has heavy tail Pq(deg f ∗ ≥ k) ∼ Cqk−α , k → ∞ where α = a − 1/2 ∈ (0, 2). Consequently, the largest face of a W n

q -disributed map has degree

  • f order n1/α.
  • G. Miermont (Orsay)

Random maps with large faces CMPP Ascona 6 / 24

slide-21
SLIDE 21

Scaling limits for Boltzmann-distributed maps

When q is ‘regular enough’ (e.g. decreasing sufficiently fast), then degrees of typical faces of a W n

q -sampled map are exponentially

  • tight. Intuitively, faces remain small:

◮ the maximal degree is of order log n, ◮ distances are still of the order n1/4. ◮ One expects the scaling limit to be still the Brownian map

[Marckert-M.,M.-Weill].

But if for some a ∈ (3/2, 5/2), we have q◦

k ∼ k−a ,

k → ∞ and qk = cβkq◦

k for the appropriate “critical” value of (c, β), then

the typical face in a Pq-sampled map has heavy tail Pq(deg f ∗ ≥ k) ∼ Cqk−α , k → ∞ where α = a − 1/2 ∈ (0, 2). Consequently, the largest face of a W n

q -disributed map has degree

  • f order n1/α.
  • G. Miermont (Orsay)

Random maps with large faces CMPP Ascona 6 / 24

slide-22
SLIDE 22

Main result

We assume qk = c q◦

k where q◦ k ∼ k−a for some a ∈ (3/2, 5/2),

c > 0 a critical value (explicit in terms of q◦). Let α = a − 1/2 ∈ (1, 2). Let Mn be a map with distribution W n

q .

Theorem

For every increasing sequence, there exists a subsequence along which (V(Mn), n−1/2αdgr)

(d)

− →

n→∞ (M∞, δ∞) ,

for the Gromov-Hausdorff topology. Moreover, the limiting space (M∞, δ∞) has Hausdorff dimension dimH(M∞, δ∞) = 2α a.s. The limit is not the Brownian map, we have a one-parameter family of pairwise distinct limit spaces. Large faces remain visible in the scaling limit, which is not a topological sphere.

  • G. Miermont (Orsay)

Random maps with large faces CMPP Ascona 7 / 24

slide-23
SLIDE 23

Main result

We assume qk = c q◦

k where q◦ k ∼ k−a for some a ∈ (3/2, 5/2),

c > 0 a critical value (explicit in terms of q◦). Let α = a − 1/2 ∈ (1, 2). Let Mn be a map with distribution W n

q .

Theorem

For every increasing sequence, there exists a subsequence along which (V(Mn), n−1/2αdgr)

(d)

− →

n→∞ (M∞, δ∞) ,

for the Gromov-Hausdorff topology. Moreover, the limiting space (M∞, δ∞) has Hausdorff dimension dimH(M∞, δ∞) = 2α a.s. The limit is not the Brownian map, we have a one-parameter family of pairwise distinct limit spaces. Large faces remain visible in the scaling limit, which is not a topological sphere.

  • G. Miermont (Orsay)

Random maps with large faces CMPP Ascona 7 / 24

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SLIDE 24

Main tool: bijective methods

A now standard tool to attack scaling limits problems on random maps is to use bijective encodings of maps by tree structures whose scaling limit is easier to determine. We use the Bouttier-Di Francesco-Guitter (BDG) bijection between rooted, pointed bipartite maps and mobiles.

−1 −2 1 −1 −2 −1 −1 −2

A mobile is a pair (T , (ℓ(v)v∈T ◦)) where T a rooted plane tree: vertices T ◦ at even generations are white, others are black T •. ℓ : T ◦ → Z is a label function with ℓ(root) = 0 and ℓ(v(i+1)) − ℓ(v(i)) ≥ −1, where v(0), v(1), . . . , v(k), v(k+1) = v(0) are the white vertices around a given black vertex, in clockwise order.

  • G. Miermont (Orsay)

Random maps with large faces CMPP Ascona 8 / 24

slide-25
SLIDE 25

Main tool: bijective methods

A now standard tool to attack scaling limits problems on random maps is to use bijective encodings of maps by tree structures whose scaling limit is easier to determine. We use the Bouttier-Di Francesco-Guitter (BDG) bijection between rooted, pointed bipartite maps and mobiles.

−1 −2 1 −1 −2 −1 −1 −2

A mobile is a pair (T , (ℓ(v)v∈T ◦)) where T a rooted plane tree: vertices T ◦ at even generations are white, others are black T •. ℓ : T ◦ → Z is a label function with ℓ(root) = 0 and ℓ(v(i+1)) − ℓ(v(i)) ≥ −1, where v(0), v(1), . . . , v(k), v(k+1) = v(0) are the white vertices around a given black vertex, in clockwise order.

  • G. Miermont (Orsay)

Random maps with large faces CMPP Ascona 8 / 24

slide-26
SLIDE 26

Main tool: bijective methods

A now standard tool to attack scaling limits problems on random maps is to use bijective encodings of maps by tree structures whose scaling limit is easier to determine. We use the Bouttier-Di Francesco-Guitter (BDG) bijection between rooted, pointed bipartite maps and mobiles.

−1 −2 1 −1 −2 −1 −1 −2

A mobile is a pair (T , (ℓ(v)v∈T ◦)) where T a rooted plane tree: vertices T ◦ at even generations are white, others are black T •. ℓ : T ◦ → Z is a label function with ℓ(root) = 0 and ℓ(v(i+1)) − ℓ(v(i)) ≥ −1, where v(0), v(1), . . . , v(k), v(k+1) = v(0) are the white vertices around a given black vertex, in clockwise order.

  • G. Miermont (Orsay)

Random maps with large faces CMPP Ascona 8 / 24

slide-27
SLIDE 27

Main tool: bijective methods

A now standard tool to attack scaling limits problems on random maps is to use bijective encodings of maps by tree structures whose scaling limit is easier to determine. We use the Bouttier-Di Francesco-Guitter (BDG) bijection between rooted, pointed bipartite maps and mobiles.

−1 −2 1 −1 −2 −1 −1 −2

A mobile is a pair (T , (ℓ(v)v∈T ◦)) where T a rooted plane tree: vertices T ◦ at even generations are white, others are black T •. ℓ : T ◦ → Z is a label function with ℓ(root) = 0 and ℓ(v(i+1)) − ℓ(v(i)) ≥ −1, where v(0), v(1), . . . , v(k), v(k+1) = v(0) are the white vertices around a given black vertex, in clockwise order.

  • G. Miermont (Orsay)

Random maps with large faces CMPP Ascona 8 / 24

slide-28
SLIDE 28

Main tool: bijective methods

A now standard tool to attack scaling limits problems on random maps is to use bijective encodings of maps by tree structures whose scaling limit is easier to determine. We use the Bouttier-Di Francesco-Guitter (BDG) bijection between rooted, pointed bipartite maps and mobiles.

−1 −2 1 −1 −2 −1 −1 −2

A mobile is a pair (T , (ℓ(v)v∈T ◦)) where T a rooted plane tree: vertices T ◦ at even generations are white, others are black T •. ℓ : T ◦ → Z is a label function with ℓ(root) = 0 and ℓ(v(i+1)) − ℓ(v(i)) ≥ −1, where v(0), v(1), . . . , v(k), v(k+1) = v(0) are the white vertices around a given black vertex, in clockwise order.

  • G. Miermont (Orsay)

Random maps with large faces CMPP Ascona 8 / 24

slide-29
SLIDE 29

Main tool: bijective methods

A now standard tool to attack scaling limits problems on random maps is to use bijective encodings of maps by tree structures whose scaling limit is easier to determine. We use the Bouttier-Di Francesco-Guitter (BDG) bijection between rooted, pointed bipartite maps and mobiles.

v(0) = v(6) v(1) v(2) v(5) ℓ(v(i+1)) − ℓ(v(i)) ≥ −1 Discrete bridge

A mobile is a pair (T , (ℓ(v)v∈T ◦)) where T a rooted plane tree: vertices T ◦ at even generations are white, others are black T •. ℓ : T ◦ → Z is a label function with ℓ(root) = 0 and ℓ(v(i+1)) − ℓ(v(i)) ≥ −1, where v(0), v(1), . . . , v(k), v(k+1) = v(0) are the white vertices around a given black vertex, in clockwise order.

  • G. Miermont (Orsay)

Random maps with large faces CMPP Ascona 8 / 24

slide-30
SLIDE 30

The BDG bijection

Start from a mobile θ = (T , ℓ) with n + 1 vertices. Let v◦

0 = root, v◦ 1, v◦ 2, . . . , v◦ n−1

be the contour exploration of white vertices, extended by periodicity to v◦

i , i ≥ 0.

Add a vertex v∗ not in T , set v◦

∞ = v∗ by convention.

For every i ≥ 0, draw an edge between v◦

i and v◦ φ(i) where

φ(i) = inf{j ≥ i : ℓ(v◦

j ) = ℓ(v◦ i )−1} .

Root the graph at the edge from v◦

φ(0) to v◦ 0.

Remove edges incident to T •.

−1 −2 1 −1 −2 −1 −1 −2

  • G. Miermont (Orsay)

Random maps with large faces CMPP Ascona 9 / 24

slide-31
SLIDE 31

The BDG bijection

Start from a mobile θ = (T , ℓ) with n + 1 vertices. Let v◦

0 = root, v◦ 1, v◦ 2, . . . , v◦ n−1

be the contour exploration of white vertices, extended by periodicity to v◦

i , i ≥ 0.

Add a vertex v∗ not in T , set v◦

∞ = v∗ by convention.

For every i ≥ 0, draw an edge between v◦

i and v◦ φ(i) where

φ(i) = inf{j ≥ i : ℓ(v◦

j ) = ℓ(v◦ i )−1} .

Root the graph at the edge from v◦

φ(0) to v◦ 0.

Remove edges incident to T •.

−1 −2 1 −1 −2 −1 −1 −2 v0 v1 v2 v3

  • G. Miermont (Orsay)

Random maps with large faces CMPP Ascona 9 / 24

slide-32
SLIDE 32

The BDG bijection

Start from a mobile θ = (T , ℓ) with n + 1 vertices. Let v◦

0 = root, v◦ 1, v◦ 2, . . . , v◦ n−1

be the contour exploration of white vertices, extended by periodicity to v◦

i , i ≥ 0.

Add a vertex v∗ not in T , set v◦

∞ = v∗ by convention.

For every i ≥ 0, draw an edge between v◦

i and v◦ φ(i) where

φ(i) = inf{j ≥ i : ℓ(v◦

j ) = ℓ(v◦ i )−1} .

Root the graph at the edge from v◦

φ(0) to v◦ 0.

Remove edges incident to T •.

−1 −2 1 −1 −2 −1 −1 −2 v0 v1 v2 v3 v10 v4 v9 v5

  • G. Miermont (Orsay)

Random maps with large faces CMPP Ascona 9 / 24

slide-33
SLIDE 33

The BDG bijection

Start from a mobile θ = (T , ℓ) with n + 1 vertices. Let v◦

0 = root, v◦ 1, v◦ 2, . . . , v◦ n−1

be the contour exploration of white vertices, extended by periodicity to v◦

i , i ≥ 0.

Add a vertex v∗ not in T , set v◦

∞ = v∗ by convention.

For every i ≥ 0, draw an edge between v◦

i and v◦ φ(i) where

φ(i) = inf{j ≥ i : ℓ(v◦

j ) = ℓ(v◦ i )−1} .

Root the graph at the edge from v◦

φ(0) to v◦ 0.

Remove edges incident to T •.

−1 −2 1 −1 −2 −1 −1 −2 v∗

  • G. Miermont (Orsay)

Random maps with large faces CMPP Ascona 9 / 24

slide-34
SLIDE 34

The BDG bijection

Start from a mobile θ = (T , ℓ) with n + 1 vertices. Let v◦

0 = root, v◦ 1, v◦ 2, . . . , v◦ n−1

be the contour exploration of white vertices, extended by periodicity to v◦

i , i ≥ 0.

Add a vertex v∗ not in T , set v◦

∞ = v∗ by convention.

For every i ≥ 0, draw an edge between v◦

i and v◦ φ(i) where

φ(i) = inf{j ≥ i : ℓ(v◦

j ) = ℓ(v◦ i )−1} .

Root the graph at the edge from v◦

φ(0) to v◦ 0.

Remove edges incident to T •.

−1 −2 1 −1 −2 −1 −1 −2 v∗

  • G. Miermont (Orsay)

Random maps with large faces CMPP Ascona 9 / 24

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SLIDE 35

The BDG bijection

Start from a mobile θ = (T , ℓ) with n + 1 vertices. Let v◦

0 = root, v◦ 1, v◦ 2, . . . , v◦ n−1

be the contour exploration of white vertices, extended by periodicity to v◦

i , i ≥ 0.

Add a vertex v∗ not in T , set v◦

∞ = v∗ by convention.

For every i ≥ 0, draw an edge between v◦

i and v◦ φ(i) where

φ(i) = inf{j ≥ i : ℓ(v◦

j ) = ℓ(v◦ i )−1} .

Root the graph at the edge from v◦

φ(0) to v◦ 0.

Remove edges incident to T •.

−1 −2 1 −1 −2 −1 −1 −2 v∗

  • G. Miermont (Orsay)

Random maps with large faces CMPP Ascona 9 / 24

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SLIDE 36

The BDG bijection

Start from a mobile θ = (T , ℓ) with n + 1 vertices. Let v◦

0 = root, v◦ 1, v◦ 2, . . . , v◦ n−1

be the contour exploration of white vertices, extended by periodicity to v◦

i , i ≥ 0.

Add a vertex v∗ not in T , set v◦

∞ = v∗ by convention.

For every i ≥ 0, draw an edge between v◦

i and v◦ φ(i) where

φ(i) = inf{j ≥ i : ℓ(v◦

j ) = ℓ(v◦ i )−1} .

Root the graph at the edge from v◦

φ(0) to v◦ 0.

Remove edges incident to T •.

−1 −2 1 −1 −2 −1 −1 −2 v∗

  • G. Miermont (Orsay)

Random maps with large faces CMPP Ascona 9 / 24

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SLIDE 37

The BDG bijection

Start from a mobile θ = (T , ℓ) with n + 1 vertices. Let v◦

0 = root, v◦ 1, v◦ 2, . . . , v◦ n−1

be the contour exploration of white vertices, extended by periodicity to v◦

i , i ≥ 0.

Add a vertex v∗ not in T , set v◦

∞ = v∗ by convention.

For every i ≥ 0, draw an edge between v◦

i and v◦ φ(i) where

φ(i) = inf{j ≥ i : ℓ(v◦

j ) = ℓ(v◦ i )−1} .

Root the graph at the edge from v◦

φ(0) to v◦ 0.

Remove edges incident to T •.

v∗

  • G. Miermont (Orsay)

Random maps with large faces CMPP Ascona 9 / 24

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SLIDE 38

Properties of the BDG bijection

3 2 1 4 3 2 1 2 2 1 3 v∗ −1 −2 1 −1 −2 −1 −1 −2

Proposition

This yields a bijection between

1

Mobiles θ = (T , ℓ), and

2

bipartite, rooted and pointed maps (m, v∗, e) such that (positivity) dgr(v∗, e−) = dgr(v∗, e+) − 1 . A vertex v ∈ T ◦ corresponds to a vertex v ∈ V(m) \ {v∗} such that dgr(v, v∗) = ℓ(v) − min ℓ + 1 A vertex v ∈ T • with k children corresponds to a face of m of degree 2k + 2.

  • G. Miermont (Orsay)

Random maps with large faces CMPP Ascona 10 / 24

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SLIDE 39

Properties of the BDG bijection

3 2 1 4 3 2 1 2 2 1 3 v∗ −1 −2 1 −1 −2 −1 −1 −2

Proposition

This yields a bijection between

1

Mobiles θ = (T , ℓ), and

2

bipartite, rooted and pointed maps (m, v∗, e) such that (positivity) dgr(v∗, e−) = dgr(v∗, e+) − 1 . A vertex v ∈ T ◦ corresponds to a vertex v ∈ V(m) \ {v∗} such that dgr(v, v∗) = ℓ(v) − min ℓ + 1 A vertex v ∈ T • with k children corresponds to a face of m of degree 2k + 2.

  • G. Miermont (Orsay)

Random maps with large faces CMPP Ascona 10 / 24

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SLIDE 40

Boltzmann distributions and the BDG bijection

Assume (M, v∗, e) has a Boltzmann distribution Pq(m, v∗, e) = Z −1

q

  • f∈F(m)

qdeg(f)/2 . Let θ = (T , ℓ) be the random mobile associated with M.

Proposition

The tree T is a Galton-Watson tree with two alternating types, and respective (white, black) offspring distributions µ0(k) = Z −1

q (1 − Z −1 q )k, k ≥ 0, and

µ1(k) = Z k

q

2k+1

k

  • qk+1

fq(Zq) , k ≥ 0. Conditionally on T , the labels ℓ are uniform among labels satisfying the constraints in the definition of mobiles.

  • G. Miermont (Orsay)

Random maps with large faces CMPP Ascona 11 / 24

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SLIDE 41

Boltzmann distributions and the BDG bijection

Assume (M, v∗, e) has a Boltzmann distribution Pq(m, v∗, e) = Z −1

q

  • f∈F(m)

qdeg(f)/2 . Let θ = (T , ℓ) be the random mobile associated with M.

Proposition

The tree T is a Galton-Watson tree with two alternating types, and respective (white, black) offspring distributions µ0(k) = Z −1

q (1 − Z −1 q )k, k ≥ 0, and

µ1(k) = Z k

q

2k+1

k

  • qk+1

fq(Zq) , k ≥ 0. Conditionally on T , the labels ℓ are uniform among labels satisfying the constraints in the definition of mobiles.

  • G. Miermont (Orsay)

Random maps with large faces CMPP Ascona 11 / 24

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SLIDE 42

Large faces in scaling limits

For an appropriate choice of qk, in the form qk = cβkq◦

k ,

q◦

k ∼ k−a ,

a ∈ (3/2, 5/2), the tree T is critical and µ1([k, ∞)) ∼ Cqk−α , k → ∞ , α = a − 1/2. This says that the degree of a typical face of M (the

  • ffspring distribution of a typical vertex of T •) is in the domain of

attraction of a stable(α) random variable. Conditioning on the number of vertices of M to be n + 1 (n the number of vertices of T ◦), the largest faces will have degrees of

  • rder n1/α and follow a Poissonian-like repartition.
  • G. Miermont (Orsay)

Random maps with large faces CMPP Ascona 12 / 24

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SLIDE 43

Key result

Let Mn have distribution W n

q , v∗ a uniformly chosen vertex in Mn,

θn = (Tn, ℓn) the associated mobile, v◦

0, v◦ 1, . . . the contour sequence.

Λθn

i

= ℓn(v◦

i ) ,

i ≥ 0 (0 for i ≥ #T ). Recall that ℓn measures distances in Mn: dgr(v◦

i , v∗) = ℓn(v◦ i ) − min ℓn + 1 = Λθn i

− Λθn + 1 .

Proposition

As n → ∞, we have the following convergence in distribution in the Skorokhod space:

  • n−1/2αΛθn

[nt], t ≥ 0

  • (d)

− →

n→∞ (Dt, t ≥ 0) ,

where (Dt, t ≥ 0) is a continuous stochastic process called the continuous distance process.

  • G. Miermont (Orsay)

Random maps with large faces CMPP Ascona 13 / 24

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SLIDE 44

Key result

Let Mn have distribution W n

q , v∗ a uniformly chosen vertex in Mn,

θn = (Tn, ℓn) the associated mobile, v◦

0, v◦ 1, . . . the contour sequence.

Λθn

i

= ℓn(v◦

i ) ,

i ≥ 0 (0 for i ≥ #T ). Recall that ℓn measures distances in Mn: dgr(v◦

i , v∗) = ℓn(v◦ i ) − min ℓn + 1 = Λθn i

− Λθn + 1 .

Proposition

As n → ∞, we have the following convergence in distribution in the Skorokhod space:

  • n−1/2αΛθn

[nt], t ≥ 0

  • (d)

− →

n→∞ (Dt, t ≥ 0) ,

where (Dt, t ≥ 0) is a continuous stochastic process called the continuous distance process.

  • G. Miermont (Orsay)

Random maps with large faces CMPP Ascona 13 / 24

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SLIDE 45

The continuous distance process

Let (Xt, 0 ≤ t ≤ 1) be the standard excursion above its minimum

  • f a stable(α) Lévy process with only positive jumps.

t s infs≤u≤t Xs Xs−

A simplifying picture (making as if X were of finite variation) With each jump of X, say s such that ∆Xs = Xs − Xs− > 0, associate an independent Brownian bridge (bs(u), 0 ≤ u ≤ ∆Xs) with duration ∆Xt. Set Dt =

  • 0<s≤t

bs

  • inf

s≤u≤t Xu − Xs−

+ Fact: D is a.s. continuous! (Even 1/(2α + ε)-Hölder)

  • G. Miermont (Orsay)

Random maps with large faces CMPP Ascona 14 / 24

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SLIDE 46

The continuous distance process

Let (Xt, 0 ≤ t ≤ 1) be the standard excursion above its minimum

  • f a stable(α) Lévy process with only positive jumps.

t s infs≤u≤t Xs Xs−

A simplifying picture (making as if X were of finite variation) With each jump of X, say s such that ∆Xs = Xs − Xs− > 0, associate an independent Brownian bridge (bs(u), 0 ≤ u ≤ ∆Xs) with duration ∆Xt. Set Dt =

  • 0<s≤t

bs

  • inf

s≤u≤t Xu − Xs−

+ Fact: D is a.s. continuous! (Even 1/(2α + ε)-Hölder)

  • G. Miermont (Orsay)

Random maps with large faces CMPP Ascona 14 / 24

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SLIDE 47

Discrete distance process

We use the coding of a tree by its Łukasiewicz path (simplifying picture: we forget about •-◦ differences between generations)

u0 u1 u2 u3

  • Lukasiewicz walk

1 2 i #{children of ui} − 1 ui

The label of u is approximately

  • v ancestor of u

bridge(length=#children(v))

rank of subtree at v containing u

  • G. Miermont (Orsay)

Random maps with large faces CMPP Ascona 15 / 24

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SLIDE 48

Discrete distance process

We use the coding of a tree by its Łukasiewicz path (simplifying picture: we forget about •-◦ differences between generations)

u0 u1 u2 u3

  • Lukasiewicz walk

1 2 i #{children of ui} − 1 ui

The label of u is approximately

  • v ancestor of u

bridge(length=#children(v))

rank of subtree at v containing u

  • G. Miermont (Orsay)

Random maps with large faces CMPP Ascona 15 / 24

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SLIDE 49

Discrete distance process (continued)

The ranks among their brothers of the ancestors of a vertex are particularly simple expressions of the Łukasiewicz walk S:

1 2 3 1 1 2 3 4 1 2 3

The label of ui is approximately

  • 1≤j≤i

bridge

(Sj−Sj−1+1) (Sj−Sj,i+1)+

where Sa,b = mina≤k≤b Sk

  • G. Miermont (Orsay)

Random maps with large faces CMPP Ascona 16 / 24

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SLIDE 50

Discrete distance process (continued)

The ranks among their brothers of the ancestors of a vertex are particularly simple expressions of the Łukasiewicz walk S:

1 2 3 1 1 2 3 4 1 2 3

The label of ui is approximately

  • 1≤j≤i

bridge

(Sj−Sj−1+1) (Sj−Sj,i+1)+

where Sa,b = mina≤k≤b Sk

  • G. Miermont (Orsay)

Random maps with large faces CMPP Ascona 16 / 24

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SLIDE 51

A motivation from physics: O(N) models

Let q be a rooted quadrangulation, i.e. a rooted (planar) map with faces all of degree 4. A loop configuration on q is a collection L = {c1, . . . , ck}, where c1, . . . , ck are simple cycles, the ci’s are non-intersecting Set #L = k and lg(L) =

k

  • i=1

lg(ci) , where lg(ci) is the number of edges in the path ci.

  • G. Miermont (Orsay)

Random maps with large faces CMPP Ascona 17 / 24

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SLIDE 52

A motivation from physics: O(N) models

Let q be a rooted quadrangulation, i.e. a rooted (planar) map with faces all of degree 4. A loop configuration on q is a collection L = {c1, . . . , ck}, where c1, . . . , ck are simple cycles, the ci’s are non-intersecting Set #L = k and lg(L) =

k

  • i=1

lg(ci) , where lg(ci) is the number of edges in the path ci.

  • G. Miermont (Orsay)

Random maps with large faces CMPP Ascona 17 / 24

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SLIDE 53

O(N) measure on random quadrangulations

Let N ≥ 0 be fixed. Let β, x > 0 be positive numbers. On the set of pairs (q, L), where

◮ q is a rooted quadrangulation ◮ L is a loop configuration on q,

we define a σ-finite measure by WO(N)(q, L) = e−β#F(q)xlg(L)N#L , the annealed O(N) measure on random quadrangulations. When the total mass is finite: ZO(N)(β, x) = WO(N)(1) < ∞ , we define a probability measure PO(N) by renormalizing WO(N) by ZO(N)(β, x).

  • G. Miermont (Orsay)

Random maps with large faces CMPP Ascona 18 / 24

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SLIDE 54

Exterior gaskets

Let (q, L) be a configuration. A cycle c ∈ L has an interior (the component of S2 \ c not containing the face incident to the root) Deleting the interior of all cycles c ∈ L, get the external gasket of E(q, L). The map E(q, L) has two types of faces: native quadrangles Q(m) and holes H(m) of any degree (shaded), with simple and mutually avoiding boundaries.

  • G. Miermont (Orsay)

Random maps with large faces CMPP Ascona 19 / 24

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SLIDE 55

Boltzmann laws induced by O(N) measures

The law of the exterior gasket of an O(N)-model on quadrangulations is WO(N)({E(q, L) = m}) = e−β#Q(m)

  • f∈H(m)

qdeg f/2 , where qk = x2kZ ∂

O(N),k(β, x) ,

where Z ∂

O(N),k(β, x) is the partition function for the O(N)-model

with a boundary of length 2k. This can be seen as a kind of Boltzmann distribution on random maps, similar to the ones studied before.

  • G. Miermont (Orsay)

Random maps with large faces CMPP Ascona 20 / 24

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SLIDE 56

Prediction from Physics

Expect (see e.g. surveys by Duplantier), for N = 2 cos(πθ) with θ ∈ (0, 1/2), that there exists xc(β) a positive function, and βc > 0 such that

◮ for given β > βc, x = xc(β), then as k → ∞

Z ∂

O(N),k(β, x) ≈ k−2+θ

◮ for β = βc, x = xc(βc), then as k → ∞

Z ∂

O(N),k(β, x) ≈ k−2−θ

respectively called dense and dilute phases. This should correspond to our models with α ∈ {3/2 − θ, 3/2 + θ}. Note the conjectured coexistence when θ = 0, N = 2. This should be related to conformal loop ensembles (Sheffield and Werner), and the KPZ formula linking models on random maps and regular lattices.

  • G. Miermont (Orsay)

Random maps with large faces CMPP Ascona 21 / 24

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SLIDE 57

Prediction from Physics

Expect (see e.g. surveys by Duplantier), for N = 2 cos(πθ) with θ ∈ (0, 1/2), that there exists xc(β) a positive function, and βc > 0 such that

◮ for given β > βc, x = xc(β), then as k → ∞

Z ∂

O(N),k(β, x) ≈ k−2+θ

◮ for β = βc, x = xc(βc), then as k → ∞

Z ∂

O(N),k(β, x) ≈ k−2−θ

respectively called dense and dilute phases. This should correspond to our models with α ∈ {3/2 − θ, 3/2 + θ}. Note the conjectured coexistence when θ = 0, N = 2. This should be related to conformal loop ensembles (Sheffield and Werner), and the KPZ formula linking models on random maps and regular lattices.

  • G. Miermont (Orsay)

Random maps with large faces CMPP Ascona 21 / 24

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SLIDE 58

Prediction from Physics

Expect (see e.g. surveys by Duplantier), for N = 2 cos(πθ) with θ ∈ (0, 1/2), that there exists xc(β) a positive function, and βc > 0 such that

◮ for given β > βc, x = xc(β), then as k → ∞

Z ∂

O(N),k(β, x) ≈ k−2+θ

◮ for β = βc, x = xc(βc), then as k → ∞

Z ∂

O(N),k(β, x) ≈ k−2−θ

respectively called dense and dilute phases. This should correspond to our models with α ∈ {3/2 − θ, 3/2 + θ}. Note the conjectured coexistence when θ = 0, N = 2. This should be related to conformal loop ensembles (Sheffield and Werner), and the KPZ formula linking models on random maps and regular lattices.

  • G. Miermont (Orsay)

Random maps with large faces CMPP Ascona 21 / 24

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SLIDE 59

The case of the Ising model

An Ising configuration is now a pair (q, σ) where q is a rooted quadrangulation, and σ = (σf, f ∈ F(q)) ∈ {−1, +1}F(q) The (annealed) Ising measure is (J a real parameter) WI(q, σ) = e−β#F(q) exp

  • J
  • f∼f ′

σfσf ′

  • ,

and define exterior gaskets in a similar fashion as for O(N) models — Note that this time, the boundaries are only weakly avoiding

+ + + + − + + + + + + + + + + + + + + + + + − + − − − − + + − − − − − − + − − − − − + −

  • G. Miermont (Orsay)

Random maps with large faces CMPP Ascona 22 / 24

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SLIDE 60

Predictions

Predictions from physics [Kazakov] identify Jc = ln 2 as critical Expects that respectively for J = Jc or J < Jc (and the appropriate values of β), the Ising model has the same scaling limit as the dilute and dense phases of the O(N = 1) model These correspond to θ = 1/3 and α ∈ {11/6, 7/6}. Need to compute generating functions for Ising model with boundary.

  • G. Miermont (Orsay)

Random maps with large faces CMPP Ascona 23 / 24

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SLIDE 61

Open problems and perspectives

1

Uniqueness of the limit laws.

2

Equivalent question: joint laws of mutual distances between k randomly sampled points.

3

Other geometric aspects of the limit (“random Sierpinsky gasket”).

4

Adding topological constraints on faces (self and mutually avoiding).

  • G. Miermont (Orsay)

Random maps with large faces CMPP Ascona 24 / 24