Scaling limits of random dissections Igor Kortchemski (work with N. - - PowerPoint PPT Presentation

scaling limits of random dissections
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Scaling limits of random dissections Igor Kortchemski (work with N. - - PowerPoint PPT Presentation

Scaling limits of random dissections Igor Kortchemski (work with N. Curien and B. Haas) DMA cole Normale Suprieure SIAM Discrete Mathematics - June 2014 Motivation Definition: Boltzmann dissections Theorem Applications Proof Outline


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Scaling limits of random dissections

Igor Kortchemski (work with N. Curien and B. Haas)

DMA – École Normale Supérieure

SIAM Discrete Mathematics - June 2014

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Motivation Definition: Boltzmann dissections Theorem Applications Proof

Outline

  • O. Motivation
  • I. Definition
  • II. Theorem
  • III. Application
  • IV. Proof

Igor Kortchemski (ÉNS Paris) Scaling limits of random dissections 2 / 475

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Motivation Definition: Boltzmann dissections Theorem Applications Proof

  • O. Motivation
  • I. Definition
  • II. Theorem
  • III. Application
  • IV. Proof

Igor Kortchemski (ÉNS Paris) Scaling limits of random dissections 3 / 475

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Motivation Definition: Boltzmann dissections Theorem Applications Proof

Scaling limits of random maps

Goal: choose a random map Mn of size n and study its global geometry as n → ∞.

Igor Kortchemski (ÉNS Paris) Scaling limits of random dissections 4 / 475

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Motivation Definition: Boltzmann dissections Theorem Applications Proof

Scaling limits of random maps

Goal: choose a random map Mn of size n and study its global geometry as n → ∞. If possible, show that a continuous limit exists (Chassaing & Schaeffer ’04).

Igor Kortchemski (ÉNS Paris) Scaling limits of random dissections 4 / 475

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Motivation Definition: Boltzmann dissections Theorem Applications Proof

Scaling limits of random maps

Goal: choose a random map Mn of size n and study its global geometry as n → ∞. If possible, show that a continuous limit exists (Chassaing & Schaeffer ’04). Problem (Schramm at ICM ’06): Let Tn be a random uniform triangulation of the sphere with n vertices.

Igor Kortchemski (ÉNS Paris) Scaling limits of random dissections 4 / 475

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SLIDE 7

Motivation Definition: Boltzmann dissections Theorem Applications Proof

Scaling limits of random maps

Goal: choose a random map Mn of size n and study its global geometry as n → ∞. If possible, show that a continuous limit exists (Chassaing & Schaeffer ’04). Problem (Schramm at ICM ’06): Let Tn be a random uniform triangulation of the sphere with n vertices. View Tn as a compact metric space.

Igor Kortchemski (ÉNS Paris) Scaling limits of random dissections 4 / 475

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Motivation Definition: Boltzmann dissections Theorem Applications Proof

Scaling limits of random maps

Goal: choose a random map Mn of size n and study its global geometry as n → ∞. If possible, show that a continuous limit exists (Chassaing & Schaeffer ’04). Problem (Schramm at ICM ’06): Let Tn be a random uniform triangulation of the sphere with n vertices. View Tn as a compact metric space. Show that n−1/4 · Tn converges towards a random compact metric space (the Brownian map)

Igor Kortchemski (ÉNS Paris) Scaling limits of random dissections 4 / 475

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Motivation Definition: Boltzmann dissections Theorem Applications Proof

Scaling limits of random maps

Goal: choose a random map Mn of size n and study its global geometry as n → ∞. If possible, show that a continuous limit exists (Chassaing & Schaeffer ’04). Problem (Schramm at ICM ’06): Let Tn be a random uniform triangulation of the sphere with n vertices. View Tn as a compact metric space. Show that n−1/4 · Tn converges towards a random compact metric space (the Brownian map), in distribution for the Gromov–Hausdorff topology.

Igor Kortchemski (ÉNS Paris) Scaling limits of random dissections 4 / 475

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Motivation Definition: Boltzmann dissections Theorem Applications Proof

Scaling limits of random maps

Goal: choose a random map Mn of size n and study its global geometry as n → ∞. If possible, show that a continuous limit exists (Chassaing & Schaeffer ’04). Problem (Schramm at ICM ’06): Let Tn be a random uniform triangulation of the sphere with n vertices. View Tn as a compact metric space. Show that n−1/4 · Tn converges towards a random compact metric space (the Brownian map), in distribution for the Gromov–Hausdorff topology. Solved by Le Gall in 2011.

Igor Kortchemski (ÉNS Paris) Scaling limits of random dissections 4 / 475

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Motivation Definition: Boltzmann dissections Theorem Applications Proof

Scaling limits of random maps

Goal: choose a random map Mn of size n and study its global geometry as n → ∞. If possible, show that a continuous limit exists (Chassaing & Schaeffer ’04). Problem (Schramm at ICM ’06): Let Tn be a random uniform triangulation of the sphere with n vertices. View Tn as a compact metric space. Show that n−1/4 · Tn converges towards a random compact metric space (the Brownian map), in distribution for the Gromov–Hausdorff topology. Solved by Le Gall in 2011. (see Le Gall’s proceeding at ICM ’14 for more information and references)

Igor Kortchemski (ÉNS Paris) Scaling limits of random dissections 4 / 475

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Motivation Definition: Boltzmann dissections Theorem Applications Proof

A simulation of the Brownian CRT

Igor Kortchemski (ÉNS Paris) Scaling limits of random dissections 5 / 475

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Motivation Definition: Boltzmann dissections Theorem Applications Proof

Random maps having the CRT as a scaling limit

Igor Kortchemski (ÉNS Paris) Scaling limits of random dissections 6 / 475

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Motivation Definition: Boltzmann dissections Theorem Applications Proof

Random maps having the CRT as a scaling limit

◮ Albenque & Marckert (’07): Uniform stack triangulations with 2n faces

Igor Kortchemski (ÉNS Paris) Scaling limits of random dissections 6 / 475

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Motivation Definition: Boltzmann dissections Theorem Applications Proof

Random maps having the CRT as a scaling limit

◮ Albenque & Marckert (’07): Uniform stack triangulations with 2n faces

Figure : Figure by Albenque & Marckert

Igor Kortchemski (ÉNS Paris) Scaling limits of random dissections 6 / 475

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Motivation Definition: Boltzmann dissections Theorem Applications Proof

Random maps having the CRT as a scaling limit

◮ Albenque & Marckert (’07): Uniform stack triangulations with 2n faces ◮ Janson & Steffánsson (’12): Boltzmann-type bipartite maps with n edges,

having a face of macroscopic degree.

Igor Kortchemski (ÉNS Paris) Scaling limits of random dissections 6 / 475

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Motivation Definition: Boltzmann dissections Theorem Applications Proof

Random maps having the CRT as a scaling limit

◮ Albenque & Marckert (’07): Uniform stack triangulations with 2n faces ◮ Janson & Steffánsson (’12): Boltzmann-type bipartite maps with n edges,

having a face of macroscopic degree.

Figure : Figure by Janson & Steffánsson

Igor Kortchemski (ÉNS Paris) Scaling limits of random dissections 6 / 475

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Motivation Definition: Boltzmann dissections Theorem Applications Proof

Random maps having the CRT as a scaling limit

◮ Albenque & Marckert (’07): Uniform stack triangulations with 2n faces ◮ Janson & Steffánsson (’12): Boltzmann-type bipartite maps with n edges,

having a face of macroscopic degree.

◮ Bettinelli (’11): Uniform quadrangulations with n faces with fixed

boundary ≫ √n.

Igor Kortchemski (ÉNS Paris) Scaling limits of random dissections 6 / 475

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Motivation Definition: Boltzmann dissections Theorem Applications Proof

  • O. Motivation
  • I. Definition: Boltzmann dissections
  • II. Theorem
  • III. Application
  • IV. Proof

Igor Kortchemski (ÉNS Paris) Scaling limits of random dissections 7 / 475

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Motivation Definition: Boltzmann dissections Theorem Applications Proof

Dissections

Let Pn be the polygon whose vertices are e

2iπj n (j = 0, 1, . . . , n − 1). Igor Kortchemski (ÉNS Paris) Scaling limits of random dissections 8 / 475

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Motivation Definition: Boltzmann dissections Theorem Applications Proof

Dissections

Let Pn be the polygon whose vertices are e

2iπj n (j = 0, 1, . . . , n − 1).

A dissection of Pn is the union of the sides Pn and of a collection of noncrossing diagonals.

Igor Kortchemski (ÉNS Paris) Scaling limits of random dissections 8 / 475

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Motivation Definition: Boltzmann dissections Theorem Applications Proof

Dissections

Let Pn be the polygon whose vertices are e

2iπj n (j = 0, 1, . . . , n − 1).

A dissection of Pn is the union of the sides Pn and of a collection of noncrossing diagonals. We will view dissections as compact metric spaces.

Igor Kortchemski (ÉNS Paris) Scaling limits of random dissections 8 / 475

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Motivation Definition: Boltzmann dissections Theorem Applications Proof

Dissections à la Boltzmann

Let Dn be the set of all dissections of Pn.

Igor Kortchemski (ÉNS Paris) Scaling limits of random dissections 9 / 147

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Motivation Definition: Boltzmann dissections Theorem Applications Proof

Dissections à la Boltzmann

Let Dn be the set of all dissections of Pn. Fix a sequence (µi)i2 of nonnegative real numbers.

Igor Kortchemski (ÉNS Paris) Scaling limits of random dissections 9 / 147

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Motivation Definition: Boltzmann dissections Theorem Applications Proof

Dissections à la Boltzmann

Let Dn be the set of all dissections of Pn. Fix a sequence (µi)i2 of nonnegative real numbers. Associate a weight π(ω) with every dissection ω ∈ Dn: π(ω) =

  • f faces of ω

µdeg(f)−1.

Igor Kortchemski (ÉNS Paris) Scaling limits of random dissections 9 / 147

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Motivation Definition: Boltzmann dissections Theorem Applications Proof

Dissections à la Boltzmann

Let Dn be the set of all dissections of Pn. Fix a sequence (µi)i2 of nonnegative real numbers. Associate a weight π(ω) with every dissection ω ∈ Dn: π(ω) =

  • f faces of ω

µdeg(f)−1.

Igor Kortchemski (ÉNS Paris) Scaling limits of random dissections 9 / 147

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Motivation Definition: Boltzmann dissections Theorem Applications Proof

Dissections à la Boltzmann

Let Dn be the set of all dissections of Pn. Fix a sequence (µi)i2 of nonnegative real numbers. Associate a weight π(ω) with every dissection ω ∈ Dn: π(ω) =

  • f faces of ω

µdeg(f)−1. Then define a probability measure on Dn by normalizing the weights: Zn =

  • ω∈Dn

π(ω) and when Zn = 0, set for every ω ∈ Dn: Pµ

n(ω) = 1

Zn π(ω).

Igor Kortchemski (ÉNS Paris) Scaling limits of random dissections 9 / 147

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Motivation Definition: Boltzmann dissections Theorem Applications Proof

Dissections à la Boltzmann

Let Dn be the set of all dissections of Pn. Fix a sequence (µi)i2 of nonnegative real numbers. Associate a weight π(ω) with every dissection ω ∈ Dn: π(ω) =

  • f faces of ω

µdeg(f)−1. Then define a probability measure on Dn by normalizing the weights: Zn =

  • ω∈Dn

π(ω) and when Zn = 0, set for every ω ∈ Dn: Pµ

n(ω) = 1

Zn π(ω). We call Pµ

n(ω) a Boltzmann probability distribution.

Igor Kortchemski (ÉNS Paris) Scaling limits of random dissections 9 / 147

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Motivation Definition: Boltzmann dissections Theorem Applications Proof

Dissections à la Boltzmann

Assume that νi = λi−1µi for every i 2 with λ > 0. Proposition.

Igor Kortchemski (ÉNS Paris) Scaling limits of random dissections 10 / 147

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Motivation Definition: Boltzmann dissections Theorem Applications Proof

Dissections à la Boltzmann

Assume that νi = λi−1µi for every i 2 with λ > 0. Then Pν

n = Pµ n.

Proposition.

Igor Kortchemski (ÉNS Paris) Scaling limits of random dissections 10 / 147

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Motivation Definition: Boltzmann dissections Theorem Applications Proof

Dissections à la Boltzmann

Assume that νi = λi−1µi for every i 2 with λ > 0. Then Pν

n = Pµ n.

Proposition. Suppose that there exists λ > 0 such that

i2 iλi−1µi = 1.

Igor Kortchemski (ÉNS Paris) Scaling limits of random dissections 10 / 147

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Motivation Definition: Boltzmann dissections Theorem Applications Proof

Dissections à la Boltzmann

Assume that νi = λi−1µi for every i 2 with λ > 0. Then Pν

n = Pµ n.

Proposition. Suppose that there exists λ > 0 such that

i2 iλi−1µi = 1. Set

ν0 = 1 −

  • i2

λi−1µi, ν1 = 0, νi = λi−1µi (i 2),

Igor Kortchemski (ÉNS Paris) Scaling limits of random dissections 10 / 147

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Motivation Definition: Boltzmann dissections Theorem Applications Proof

Dissections à la Boltzmann

Assume that νi = λi−1µi for every i 2 with λ > 0. Then Pν

n = Pµ n.

Proposition. Suppose that there exists λ > 0 such that

i2 iλi−1µi = 1. Set

ν0 = 1 −

  • i2

λi−1µi, ν1 = 0, νi = λi−1µi (i 2), Then Pν

n = Pµ n and ν is a critical probability measure on Z+ with ν1 = 0.

Igor Kortchemski (ÉNS Paris) Scaling limits of random dissections 10 / 147

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Motivation Definition: Boltzmann dissections Theorem Applications Proof

Dissections à la Boltzmann: examples

◮ Uniform p-angulations (p 3). Set

µ(p) = 1 − 1 p − 1, µ(p)

p−1 =

1 p − 1, µ(p)

i

= 0 (i = 0, i = p − 1).

Igor Kortchemski (ÉNS Paris) Scaling limits of random dissections 11 / 147

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Motivation Definition: Boltzmann dissections Theorem Applications Proof

Dissections à la Boltzmann: examples

◮ Uniform p-angulations (p 3). Set

µ(p) = 1 − 1 p − 1, µ(p)

p−1 =

1 p − 1, µ(p)

i

= 0 (i = 0, i = p − 1). Then Pµ(p)

n

is the uniform measure over all p-angulations of Pn.

Igor Kortchemski (ÉNS Paris) Scaling limits of random dissections 11 / 147

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Motivation Definition: Boltzmann dissections Theorem Applications Proof

Dissections à la Boltzmann: examples

◮ Uniform p-angulations (p 3). Set

µ(p) = 1 − 1 p − 1, µ(p)

p−1 =

1 p − 1, µ(p)

i

= 0 (i = 0, i = p − 1). Then Pµ(p)

n

is the uniform measure over all p-angulations of Pn.

◮ Uniform dissections. Set

µ0 = 2 − √ 2, µ1 = 0, µi =

  • 2 −

√ 2 2 i−1 i 2,

Igor Kortchemski (ÉNS Paris) Scaling limits of random dissections 11 / 147

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Motivation Definition: Boltzmann dissections Theorem Applications Proof

Dissections à la Boltzmann: examples

◮ Uniform p-angulations (p 3). Set

µ(p) = 1 − 1 p − 1, µ(p)

p−1 =

1 p − 1, µ(p)

i

= 0 (i = 0, i = p − 1). Then Pµ(p)

n

is the uniform measure over all p-angulations of Pn.

◮ Uniform dissections. Set

µ0 = 2 − √ 2, µ1 = 0, µi =

  • 2 −

√ 2 2 i−1 i 2, then Pµ

n is the uniform measure on the set of all dissections of Pn.

Igor Kortchemski (ÉNS Paris) Scaling limits of random dissections 11 / 147

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Motivation Definition: Boltzmann dissections Theorem Applications Proof

  • I. Definition
  • II. Theorem: scaling limits of random dissections
  • III. Application
  • IV. Proof

Igor Kortchemski (ÉNS Paris) Scaling limits of random dissections 12 / 147

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Motivation Definition: Boltzmann dissections Theorem Applications Proof

Scaling limit of random dissections

Let µ be a probability measure over {0, 2, 3, . . .} of mean 1 s.t.

i0 eλiµi < ∞

for some λ > 0.

Igor Kortchemski (ÉNS Paris) Scaling limits of random dissections 13 /

  • 8/3
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Motivation Definition: Boltzmann dissections Theorem Applications Proof

Scaling limit of random dissections

Let µ be a probability measure over {0, 2, 3, . . .} of mean 1 s.t.

i0 eλiµi < ∞

for some λ > 0. Let Dµ

n be a random dissection distributed according to Pµ n.

Igor Kortchemski (ÉNS Paris) Scaling limits of random dissections 13 /

  • 8/3
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Motivation Definition: Boltzmann dissections Theorem Applications Proof

Scaling limit of random dissections

Let µ be a probability measure over {0, 2, 3, . . .} of mean 1 s.t.

i0 eλiµi < ∞

for some λ > 0. Let Dµ

n be a random dissection distributed according to Pµ n.

What does Dµ

n look like, for n large, as a metric space?

Igor Kortchemski (ÉNS Paris) Scaling limits of random dissections 13 /

  • 8/3
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Motivation Definition: Boltzmann dissections Theorem Applications Proof

Simulations

Figure : A uniform dissection of P45.

Igor Kortchemski (ÉNS Paris) Scaling limits of random dissections 14 /

  • 8/3
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Motivation Definition: Boltzmann dissections Theorem Applications Proof

Simulations

Figure : A uniform dissection of P260.

Igor Kortchemski (ÉNS Paris) Scaling limits of random dissections 14 /

  • 8/3
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Motivation Definition: Boltzmann dissections Theorem Applications Proof

Simulations

Figure : A uniform dissection of P387.

Igor Kortchemski (ÉNS Paris) Scaling limits of random dissections 14 /

  • 8/3
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Motivation Definition: Boltzmann dissections Theorem Applications Proof

Simulations

Figure : A uniform dissection of P637.

Igor Kortchemski (ÉNS Paris) Scaling limits of random dissections 14 /

  • 8/3
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Motivation Definition: Boltzmann dissections Theorem Applications Proof

Simulations

Figure : A uniform dissection of P8916.

Igor Kortchemski (ÉNS Paris) Scaling limits of random dissections 14 /

  • 8/3
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Motivation Definition: Boltzmann dissections Theorem Applications Proof

Scaling limit of random dissections

Let µ be a probability measure over {0, 2, 3, . . .} of mean 1 s.t.

i0 eλiµi < ∞

for some λ > 0. Let Dµ

n be a random dissection distributed according to Pµ n.

Igor Kortchemski (ÉNS Paris) Scaling limits of random dissections 15 /

  • 8/3
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Motivation Definition: Boltzmann dissections Theorem Applications Proof

Scaling limit of random dissections

Let µ be a probability measure over {0, 2, 3, . . .} of mean 1 s.t.

i0 eλiµi < ∞

for some λ > 0. Let Dµ

n be a random dissection distributed according to Pµ n.

There exists a constant c(µ) such that: 1 √n · Dµ

n (d)

− − − →

n→∞

c(µ) · Te, Theorem (Curien, Haas & K.).

Igor Kortchemski (ÉNS Paris) Scaling limits of random dissections 15 /

  • 8/3
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Motivation Definition: Boltzmann dissections Theorem Applications Proof

Scaling limit of random dissections

Let µ be a probability measure over {0, 2, 3, . . .} of mean 1 s.t.

i0 eλiµi < ∞

for some λ > 0. Let Dµ

n be a random dissection distributed according to Pµ n.

There exists a constant c(µ) such that: 1 √n · Dµ

n (d)

− − − →

n→∞

c(µ) · Te, where Te is a random compact metric space, called the Brownian CRT Theorem (Curien, Haas & K.).

Igor Kortchemski (ÉNS Paris) Scaling limits of random dissections 15 /

  • 8/3
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Motivation Definition: Boltzmann dissections Theorem Applications Proof

Scaling limit of random dissections

Let µ be a probability measure over {0, 2, 3, . . .} of mean 1 s.t.

i0 eλiµi < ∞

for some λ > 0. Let Dµ

n be a random dissection distributed according to Pµ n.

There exists a constant c(µ) such that: 1 √n · Dµ

n (d)

− − − →

n→∞

c(µ) · Te, where Te is a random compact metric space, called the Brownian CRT and the convergence holds in distribution for the Gromov–Hausdorff topology

  • n compact metric spaces.

Theorem (Curien, Haas & K.).

Igor Kortchemski (ÉNS Paris) Scaling limits of random dissections 15 /

  • 8/3
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Motivation Definition: Boltzmann dissections Theorem Applications Proof

Scaling limit of random dissections

Let µ be a probability measure over {0, 2, 3, . . .} of mean 1 s.t.

i0 eλiµi < ∞

for some λ > 0. Let Dµ

n be a random dissection distributed according to Pµ n.

There exists a constant c(µ) such that: 1 √n · Dµ

n (d)

− − − →

n→∞

c(µ) · Te, where Te is a random compact metric space, called the Brownian CRT and the convergence holds in distribution for the Gromov–Hausdorff topology

  • n compact metric spaces.

In addition, c(µ) = 2 σ√µ0 · 1 4

  • σ2 +

µ0µ2Z+ 2µ2Z+ − µ0

  • ,

Theorem (Curien, Haas & K.).

Igor Kortchemski (ÉNS Paris) Scaling limits of random dissections 15 /

  • 8/3
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SLIDE 52

Motivation Definition: Boltzmann dissections Theorem Applications Proof

Scaling limit of random dissections

Let µ be a probability measure over {0, 2, 3, . . .} of mean 1 s.t.

i0 eλiµi < ∞

for some λ > 0. Let Dµ

n be a random dissection distributed according to Pµ n.

There exists a constant c(µ) such that: 1 √n · Dµ

n (d)

− − − →

n→∞

c(µ) · Te, where Te is a random compact metric space, called the Brownian CRT and the convergence holds in distribution for the Gromov–Hausdorff topology

  • n compact metric spaces.

In addition, c(µ) = 2 σ√µ0 · 1 4

  • σ2 +

µ0µ2Z+ 2µ2Z+ − µ0

  • ,

where µ2Z+ = µ0 + µ2 + µ4 + · · · and σ2 ∈ (0, ∞) is the variance of µ. Theorem (Curien, Haas & K.).

Igor Kortchemski (ÉNS Paris) Scaling limits of random dissections 15 /

  • 8/3
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SLIDE 53

Motivation Definition: Boltzmann dissections Theorem Applications Proof

What is the Brownian Continuum Random Tree?

First define the contour function of a tree:

Igor Kortchemski (ÉNS Paris) Scaling limits of random dissections 16 / −i

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Motivation Definition: Boltzmann dissections Theorem Applications Proof

What is the Brownian Continuum Random Tree?

Knowing the contour function, it is easy to recover the tree by gluing:

Igor Kortchemski (ÉNS Paris) Scaling limits of random dissections 17 / −i

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Motivation Definition: Boltzmann dissections Theorem Applications Proof

What is the Brownian Continuum Random Tree?

The Brownian tree Te is obtained by gluing from the Brownian excursion e.

0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1 0.05 0.1 0.15 0.2 0.25 0.3 0.35 0.4 0.45

Figure : A simulation of e.

Igor Kortchemski (ÉNS Paris) Scaling limits of random dissections 18 / √ 17

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Motivation Definition: Boltzmann dissections Theorem Applications Proof

A simulation of the Brownian CRT

Figure : A non isometric plane embedding of a realization of Te.

Igor Kortchemski (ÉNS Paris) Scaling limits of random dissections 19 / √ 17

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Motivation Definition: Boltzmann dissections Theorem Applications Proof

Recap

Let µ be a probability measure over {0, 2, 3, . . .} of mean 1 s.t.

i0 eλiµi < ∞

for some λ > 0. Let Dµ

n be a random dissection distributed according to Pµ n.

There exists a constant c(µ) such that: 1 √n · Dµ

n (d)

− − − →

n→∞

c(µ) · Te, where Te is a random compact metric space, called the Brownian CRT and the convergence holds in distribution for the Gromov–Hausdorff topology

  • n compact metric spaces.

In addition, c(µ) = 2 σ√µ0 · 1 4

  • σ2 +

µ0µ2Z+ 2µ2Z+ − µ0

  • ,

where µ2Z+ = µ0 + µ2 + µ4 + · · · and σ2 ∈ (0, ∞) is the variance of µ. Theorem (Curien, Haas & K.).

Igor Kortchemski (ÉNS Paris) Scaling limits of random dissections 20 / √ 17

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SLIDE 58

Motivation Definition: Boltzmann dissections Theorem Applications Proof

  • I. Definition
  • II. Theorem
  • III. Combinatorial applications
  • IV. Proof

Igor Kortchemski (ÉNS Paris) Scaling limits of random dissections 21 / √ 17

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SLIDE 59

Motivation Definition: Boltzmann dissections Theorem Applications Proof

Applications

Combinatorial properties of random dissections have been studied by various authors :

◮ Uniform triangulations : Devroye, Flajolet, Hurtado, Noy & Steiger

(maximal degree, longest diagonal, 1999) and Gao & Wormald (maximal degree, 2000),

◮ Uniform dissections (and triangulations) : Bernasconi, Panagiotou & Steger

(degrees, maximal degree, 2010) and Drmota, de Mier & Noy (diameter, 2012).

Igor Kortchemski (ÉNS Paris) Scaling limits of random dissections 22 / ?

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Motivation Definition: Boltzmann dissections Theorem Applications Proof

Applications

Combinatorial properties of random dissections have been studied by various authors :

◮ Uniform triangulations : Devroye, Flajolet, Hurtado, Noy & Steiger

(maximal degree, longest diagonal, 1999) and Gao & Wormald (maximal degree, 2000),

◮ Uniform dissections (and triangulations) : Bernasconi, Panagiotou & Steger

(degrees, maximal degree, 2010) and Drmota, de Mier & Noy (diameter, 2012).

  • When µi ∼ c/i1+α as i → ∞, loops remain in the scaling limit, which is

the stable looptree of index α ∈ (1, 2) (Curien & K.).

Igor Kortchemski (ÉNS Paris) Scaling limits of random dissections 22 / ?

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SLIDE 61

Motivation Definition: Boltzmann dissections Theorem Applications Proof

Applications

Combinatorial properties of random dissections have been studied by various authors :

◮ Uniform triangulations : Devroye, Flajolet, Hurtado, Noy & Steiger

(maximal degree, longest diagonal, 1999) and Gao & Wormald (maximal degree, 2000),

◮ Uniform dissections (and triangulations) : Bernasconi, Panagiotou & Steger

(degrees, maximal degree, 2010) and Drmota, de Mier & Noy (diameter, 2012).

  • When µi ∼ c/i1+α as i → ∞, loops remain in the scaling limit, which is

the stable looptree of index α ∈ (1, 2) (Curien & K.). The looptree of index α = 3/2 describes the scaling limit of boundaries of critical site percolation on the Uniform Infinite Planar Triangulation (Curien & K.).

Igor Kortchemski (ÉNS Paris) Scaling limits of random dissections 22 / ?

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Motivation Definition: Boltzmann dissections Theorem Applications Proof

Applications

The diameter Diam(Dµ

n) is the maximal distance between two points of Dµ n.

Igor Kortchemski (ÉNS Paris) Scaling limits of random dissections 23 / −34

slide-63
SLIDE 63

Motivation Definition: Boltzmann dissections Theorem Applications Proof

Applications

The diameter Diam(Dµ

n) is the maximal distance between two points of Dµ n.

We have for every p > 0: E

  • Diam(Dµ

n)p

n→∞

. Corollary.

Igor Kortchemski (ÉNS Paris) Scaling limits of random dissections 23 / −34

slide-64
SLIDE 64

Motivation Definition: Boltzmann dissections Theorem Applications Proof

Applications

The diameter Diam(Dµ

n) is the maximal distance between two points of Dµ n.

We have for every p > 0: E

  • Diam(Dµ

n)p

n→∞

· np/2. Corollary.

Igor Kortchemski (ÉNS Paris) Scaling limits of random dissections 23 / −34

slide-65
SLIDE 65

Motivation Definition: Boltzmann dissections Theorem Applications Proof

Applications

The diameter Diam(Dµ

n) is the maximal distance between two points of Dµ n.

We have for every p > 0: E

  • Diam(Dµ

n)p

n→∞

c(µ)p · · np/2. Corollary.

Igor Kortchemski (ÉNS Paris) Scaling limits of random dissections 23 / −34

slide-66
SLIDE 66

Motivation Definition: Boltzmann dissections Theorem Applications Proof

Applications

The diameter Diam(Dµ

n) is the maximal distance between two points of Dµ n.

We have for every p > 0: E

  • Diam(Dµ

n)p

n→∞

c(µ)p · ∞ xpfD(x)dx · np/2. Corollary.

Igor Kortchemski (ÉNS Paris) Scaling limits of random dissections 23 / −34

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SLIDE 67

Motivation Definition: Boltzmann dissections Theorem Applications Proof

Applications

The diameter Diam(Dµ

n) is the maximal distance between two points of Dµ n.

We have for every p > 0: E

  • Diam(Dµ

n)p

n→∞

c(µ)p · ∞ xpfD(x)dx · np/2. Corollary. where, setting bk,x = (16πk/x)2, fD(x) is

√ 2π 3

times

  • k1

29 x4

  • 4b4

k,x − 36b3 k,x + 75b2 k,x − 30bk,x

  • + 24

x2

  • 4b3

k,x − 10b2 k,x

  • e−bk,x.

Igor Kortchemski (ÉNS Paris) Scaling limits of random dissections 23 / −34

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SLIDE 68

Motivation Definition: Boltzmann dissections Theorem Applications Proof

Applications

The diameter Diam(Dµ

n) is the maximal distance between two points of Dµ n.

We have for every p > 0: E

  • Diam(Dµ

n)p

n→∞

c(µ)p · ∞ xpfD(x)dx · np/2. In particular, for p = 1, E

  • Diam(Dµ

n)

n→∞

c(µ) · 2 √ 2π 3 · √n. Corollary. where, setting bk,x = (16πk/x)2, fD(x) is

√ 2π 3

times

  • k1

29 x4

  • 4b4

k,x − 36b3 k,x + 75b2 k,x − 30bk,x

  • + 24

x2

  • 4b3

k,x − 10b2 k,x

  • e−bk,x.

Igor Kortchemski (ÉNS Paris) Scaling limits of random dissections 23 / −34

slide-69
SLIDE 69

Motivation Definition: Boltzmann dissections Theorem Applications Proof

Applications

The diameter Diam(Dµ

n) is the maximal distance between two points of Dµ n.

We have for every p > 0: E

  • Diam(Dµ

n)p

n→∞

c(µ)p · ∞ xpfD(x)dx · np/2. In particular, for p = 1, E

  • Diam(Dµ

n)

n→∞

c(µ) · 2 √ 2π 3 · √n. Corollary.

  • Remark: c(µ) is explicit for p-angulations and uniform dissections.

Igor Kortchemski (ÉNS Paris) Scaling limits of random dissections 23 / −34

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SLIDE 70

Motivation Definition: Boltzmann dissections Theorem Applications Proof

Applications

The diameter Diam(Dµ

n) is the maximal distance between two points of Dµ n.

We have for every p > 0: E

  • Diam(Dµ

n)p

n→∞

c(µ)p · ∞ xpfD(x)dx · np/2. In particular, for p = 1, E

  • Diam(Dµ

n)

n→∞

c(µ) · 2 √ 2π 3 · √n. Corollary.

  • Remark: c(µ) is explicit for p-angulations and uniform dissections. For

instance, for uniform dissections: c(µ) = 1 7(3 + √ 2)23/4.

Igor Kortchemski (ÉNS Paris) Scaling limits of random dissections 23 / −34

slide-71
SLIDE 71

Motivation Definition: Boltzmann dissections Theorem Applications Proof

Applications

The diameter Diam(Dµ

n) is the maximal distance between two points of Dµ n.

We have for every p > 0: E

  • Diam(Dµ

n)p

n→∞

c(µ)p · ∞ xpfD(x)dx · np/2. In particular, for p = 1, E

  • Diam(Dµ

n)

n→∞

c(µ) · 2 √ 2π 3 · √n. Corollary. For uniform dissections, we get E

  • Diam(Dµ

n)

  • ∼ 1

21(3 + √ 2)29/4 √πn ≃ 0.99988√πn.

Igor Kortchemski (ÉNS Paris) Scaling limits of random dissections 23 / −34

slide-72
SLIDE 72

Motivation Definition: Boltzmann dissections Theorem Applications Proof

Applications

The diameter Diam(Dµ

n) is the maximal distance between two points of Dµ n.

We have for every p > 0: E

  • Diam(Dµ

n)p

n→∞

c(µ)p · ∞ xpfD(x)dx · np/2. In particular, for p = 1, E

  • Diam(Dµ

n)

n→∞

c(µ) · 2 √ 2π 3 · √n. Corollary. For uniform dissections, we get E

  • Diam(Dµ

n)

  • ∼ 1

21(3 + √ 2)29/4 √πn ≃ 0.99988√πn. This strenghtens a result of Drmota, de Mier & Noy who proved that (3 + √ 2)21/4 7 √πn E

  • Diam(Dµ

n)

  • 2 · (3 +

√ 2)21/4 7 √πn ≃ 0.74√πn ≃ 1.5√πn.

Igor Kortchemski (ÉNS Paris) Scaling limits of random dissections 23 / −34

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SLIDE 73

Motivation Definition: Boltzmann dissections Theorem Applications Proof

  • I. Definition
  • II. Theorem
  • III. Application
  • IV. Proof

Igor Kortchemski (ÉNS Paris) Scaling limits of random dissections 24 / −34

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SLIDE 74

Motivation Definition: Boltzmann dissections Theorem Applications Proof

Proof

g Step 1. Consider the dual tree of Dµ

n:

Figure : A dissection and its dual tree Tµ

n.

Igor Kortchemski (ÉNS Paris) Scaling limits of random dissections 25 / ℵ0

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SLIDE 75

Motivation Definition: Boltzmann dissections Theorem Applications Proof

Proof

g Step 1. Consider the dual tree of Dµ

n:

Figure : A dissection and its dual tree Tµ

n.

Key fact. Tµ

n is a (planted) Galton–Watson tree with offspring distribution

µ conditioned on having n − 1 leaves.

Igor Kortchemski (ÉNS Paris) Scaling limits of random dissections 25 / ℵ0

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SLIDE 76

Motivation Definition: Boltzmann dissections Theorem Applications Proof

Proof

g Step 1. Consider the dual tree of Dµ

n:

Figure : A dissection and its dual tree Tµ

n.

Key fact. Tµ

n is a (planted) Galton–Watson tree with offspring distribution

µ conditioned on having n − 1 leaves. It is known (Rizzolo or K.) that: 1 √n · Tµ

n (d)

− →

n→∞

2 σ√µ0 · Te.

Igor Kortchemski (ÉNS Paris) Scaling limits of random dissections 25 / ℵ0

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SLIDE 77

Motivation Definition: Boltzmann dissections Theorem Applications Proof

Proof

g Step 2. We show that: Dµ

n

≃ 1 4

  • σ2 +

µ0µ2Z+ 2µ2Z+ − µ0

  • · Tµ

n.

Igor Kortchemski (ÉNS Paris) Scaling limits of random dissections 26 / ℵ1

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SLIDE 78

Motivation Definition: Boltzmann dissections Theorem Applications Proof

Proof

g Step 2. We show that: Dµ

n

≃ 1 4

  • σ2 +

µ0µ2Z+ 2µ2Z+ − µ0

  • · Tµ

n.

To this end, we compare the length of geodesics in Dµ

n and in Tµ n by using an

“exploration” Markov Chain:

Figure : A geodesic in Tµ

n (in light blue) and the associated geodesic in Dµ n (in red).

  • Igor Kortchemski (ÉNS Paris)

Scaling limits of random dissections 26 / ℵ1

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SLIDE 79

Motivation Definition: Boltzmann dissections Theorem Applications Proof

The Markov Chain

Igor Kortchemski (ÉNS Paris) Scaling limits of random dissections

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SLIDE 80

Motivation Definition: Boltzmann dissections Theorem Applications Proof

The Markov Chain

Igor Kortchemski (ÉNS Paris) Scaling limits of random dissections

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SLIDE 81

Motivation Definition: Boltzmann dissections Theorem Applications Proof

The Markov Chain

Igor Kortchemski (ÉNS Paris) Scaling limits of random dissections

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SLIDE 82

Motivation Definition: Boltzmann dissections Theorem Applications Proof

The Markov Chain

Igor Kortchemski (ÉNS Paris) Scaling limits of random dissections

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SLIDE 83

Motivation Definition: Boltzmann dissections Theorem Applications Proof

The Markov Chain

Igor Kortchemski (ÉNS Paris) Scaling limits of random dissections

slide-84
SLIDE 84

Motivation Definition: Boltzmann dissections Theorem Applications Proof

The Markov Chain

Igor Kortchemski (ÉNS Paris) Scaling limits of random dissections

slide-85
SLIDE 85

Motivation Definition: Boltzmann dissections Theorem Applications Proof

The Markov Chain

Igor Kortchemski (ÉNS Paris) Scaling limits of random dissections