Bijective approach to percolation on triangulations and Liouville - - PowerPoint PPT Presentation

bijective approach to percolation on triangulations and
SMART_READER_LITE
LIVE PREVIEW

Bijective approach to percolation on triangulations and Liouville - - PowerPoint PPT Presentation

Bijective approach to percolation on triangulations and Liouville quantum gravity Olivier Bernardi - Brandeis University Joint work with Nina Holden & Xin Sun MIT, March 2019 Percolation on triangulation CLE on Liouville Quantum Gravity


slide-1
SLIDE 1

Bijective approach to percolation on triangulations and Liouville quantum gravity

MIT, March 2019 Olivier Bernardi - Brandeis University Joint work with Nina Holden & Xin Sun

slide-2
SLIDE 2

Percolation on triangulation CLE on Liouville Quantum Gravity

slide-3
SLIDE 3

Percolation on triangulation CLE on Liouville Quantum Gravity “Random curves on a random surface”

slide-4
SLIDE 4

Percolation on triangulation CLE on Liouville Quantum Gravity Kreweras excursion 2D Brownian excursion

slide-5
SLIDE 5

Percolation on triangulations

slide-6
SLIDE 6

Percolation on a regular lattice Triangular lattice

slide-7
SLIDE 7

Percolation on a regular lattice Site percolation: Color vertices black or white with probability 1/2.

slide-8
SLIDE 8

Percolation on a regular lattice Questions:

  • Crossing probabilities?

A n × B n box Site percolation: Color vertices black or white with probability 1/2.

slide-9
SLIDE 9

Percolation on a regular lattice Questions:

  • Crossing probabilities?
  • Law of interfaces?

Site percolation: Color vertices black or white with probability 1/2.

  • Crossing probabilities?
slide-10
SLIDE 10

Percolation on a regular lattice Questions:

  • Crossing probabilities?
  • Law of interfaces?
  • Mixing properties?

Site percolation: Color vertices black or white with probability 1/2.

  • Crossing probabilities?
slide-11
SLIDE 11

Triangulations (of the disk)

  • Def. A triangulation of the disk is a decomposition into triangles.
slide-12
SLIDE 12

Triangulations (of the disk) =

  • Def. A triangulation of the disk is a decomposition into triangles

(considered up to deformation).

slide-13
SLIDE 13

Triangulations (of the disk) (multiple edges allowed, loops forbidden)

  • Def. A triangulation of the disk is a decomposition into triangles

(considered up to deformation).

slide-14
SLIDE 14

Triangulations (of the disk)

  • Def. A triangulation is rooted by marking an edge on the boundary.
  • Def. A triangulation of the disk is a decomposition into triangles

(considered up to deformation).

slide-15
SLIDE 15

Percolation on triangulations We can consider percolation on random triangulations of the disk. (k exterior vertices, n interior vertices; uniform probability)

slide-16
SLIDE 16

Percolation on triangulations Same questions:

  • Crossing probabilities?
  • Law of interfaces?
  • Mixing properties?

We can consider percolation on random triangulations of the disk. (k exterior vertices, n interior vertices; uniform probability)

slide-17
SLIDE 17

We can also consider infinite triangulations. Percolation on triangulations Same questions:

  • Crossing probabilities?
  • Law of interfaces?
  • Mixing properties?

We can consider percolation on random triangulations of the disk. (k exterior vertices, n interior vertices; uniform probability) Uniform Infinite Planar Triangulation [Angel,Schramm 04]

slide-18
SLIDE 18

Uniformly random triangulation with n triangles of side length n−1/4. Triangulations as a random surface

random triangulation

(image by N. Curien)

slide-19
SLIDE 19

Uniformly random triangulation with n triangles of side length n−1/4. Triangulations as a random surface

random triangulation Brownian map

(image by N. Curien)

Theorem [LeGall 2013, Miermont 2013]∗ Convergence in law as a metric space (Gromov-Hausdorff topology). Limit is random compact metric space (homeomorphic to 2D sphere) of Hausdorff dimension 4.

(∗ for a different family of planar maps)

slide-20
SLIDE 20

Regular lattices Vs random lattices Is it interesting to make statistical mechanics on random lattices?

slide-21
SLIDE 21

Regular lattices Vs random lattices Is it interesting to make statistical mechanics on random lattices? Vs regular lattice random lattice

slide-22
SLIDE 22

Regular lattices Vs random lattices Yes! The “critical exponents” on regular Vs random lattices are related by KPZ formula [Knizhnik, Polyakov, Zamolodchikov]. Is it interesting to make statistical mechanics on random lattices? Vs regular lattice random lattice

slide-23
SLIDE 23

Regular lattices Vs random lattices Yes! The “critical exponents” on regular Vs random lattices are related by KPZ formula [Knizhnik, Polyakov, Zamolodchikov]. Yes! Critically weighted triangulations family of random surfaces. Is it interesting to make statistical mechanics on random lattices? Vs regular lattice random lattice

slide-24
SLIDE 24

Liouville Quantum Gravity (LQG) and Schramm–Loewner Evolution (SLE)

slide-25
SLIDE 25

What is . . . Liouville Quantum Gravity?

slide-26
SLIDE 26

What is . . . Liouville Quantum Gravity? LQG is a random area measure µ on a C-domain related to the Gaussian free field

(image by J. Miller)

slide-27
SLIDE 27

What is . . . Liouville Quantum Gravity? 1D LQG Brownian motion 1 1D LQG 1

h µ = eγhdx

slide-28
SLIDE 28

What is . . . Liouville Quantum Gravity?

Random function chosen with probability proportional to e −

n

  • i=1

(h(i) − h(i − 1))2 2

Brownian motion 1D LQG 1D LQG

hn : [n] → R µ = eγhdx

1

h = lim hn

1 n

slide-29
SLIDE 29

What is . . . Liouville Quantum Gravity?

hn : [n]2 → R µ = eγhdxdy h = lim hn Random function chosen with probability proportional to e −

  • u∼v

(h(u) − h(v))2 2

Gaussian Free Field LQG

(a distribution) (area measure)

slide-30
SLIDE 30

What is . . . Liouville Quantum Gravity?

hn : [n]2 → R µ = eγhdxdy h = lim hn γ ∈ [0, 2] controls how wild LQG measure is. Today: γ =

  • 8/3.

”pure gravity”

slide-31
SLIDE 31

What is... a SLE (Schramm–Loewner evolution)?

slide-32
SLIDE 32

What is... a SLE (Schramm–Loewner evolution)? SLEκ is a random (non-crossing, parametrized) curve in a C-domain.

slide-33
SLIDE 33

What is... a SLE (Schramm–Loewner evolution)? SLEκ were introduced to describe the scaling limit of curves from statistical mechanics. SLEκ is a random (non-crossing, parametrized) curve in a C-domain. The parameter κ determines how much the curve “wiggles”.

slide-34
SLIDE 34

What is... a SLE (Schramm–Loewner evolution)? SLE are characterized by:

  • Conformal invariance property
  • Markov domain property

1

slide-35
SLIDE 35

What is... a SLE (Schramm–Loewner evolution)? SLE are characterized by:

  • Conformal invariance property
  • Markov domain property

1 1 φ conformal

slide-36
SLIDE 36

What is... a SLE (Schramm–Loewner evolution)? SLE are characterized by:

  • Conformal invariance property
  • Markov domain property

1 1 ei√κW (t)

γ(t) Brownian

˜ φ conformal

slide-37
SLIDE 37

What is... a SLE (Schramm–Loewner evolution)? Today: κ = 6 (percolation – characterized by target invariance)

slide-38
SLIDE 38

What is... a SLE (Schramm–Loewner evolution)? Today: κ = 6 (percolation – characterized by target invariance) Theorem [Smirnov 01]: Convergence. SLE6

slide-39
SLIDE 39

What is... a SLE (Schramm–Loewner evolution)? Today: κ = 6 (percolation – characterized by target invariance) Theorem [Smirnov 01]: Convergence.

slide-40
SLIDE 40

What is... a SLE (Schramm–Loewner evolution)? CLE6

Conformal Loop Ensemble

Today: κ = 6 (percolation – characterized by target invariance) Theorem [Smirnov 01]: Convergence. Theorem [Camia, Newman 09]: Convergence.

slide-41
SLIDE 41

The big conjecture

slide-42
SLIDE 42

The big conjecture LQG was introduced in physics as a model of random surface describing space-time evolution of strings.

Riemann surface Riemann mapping

slide-43
SLIDE 43

The big conjecture

Riemann mapping

Related?

Nice embedding

slide-44
SLIDE 44

The big conjecture

Riemann mapping

Related?

Nice embedding [Miller, Sheffield 2016]: Equality as metric spaces

slide-45
SLIDE 45

The big conjecture

Riemann mapping

Related?

Nice embedding

slide-46
SLIDE 46

Convergence results

Percolation on random triangulation CLE on Liouville Quantum Gravity

slide-47
SLIDE 47

Convergence results

Percolation on random triangulation CLE on Liouville Quantum Gravity under nice embedding some

slide-48
SLIDE 48

Thm [Bernardi, Holden, Sun]: Let (Mn, σn) uniformly random percolated triangulation of size n (n interior vertices, √n exterior vertices). There exist embeddings φn : Mn → D (and coupling) such that the following converge jointly in probability:

slide-49
SLIDE 49

Thm [Bernardi, Holden, Sun]: Let (Mn, σn) uniformly random percolated triangulation of size n (n interior vertices, √n exterior vertices). There exist embeddings φn : Mn → D (and coupling) such that the following converge jointly in probability:

  • Area measure: vertex counting measure −

  • 8/3-LQG µ.

φn(Mn) LQG√

8/3

weak topology

slide-50
SLIDE 50

Thm [Bernardi, Holden, Sun]: Let (Mn, σn) uniformly random percolated triangulation of size n (n interior vertices, √n exterior vertices). There exist embeddings φn : Mn → D (and coupling) such that the following converge jointly in probability:

  • Area measure: vertex counting measure −

  • 8/3-LQG µ.

φn(Mn, σn) LQG√

8/3 +

independent CLE6

  • Percolation cycles:

embedded percolation cycles γn

1 , γn 2 , . . .

− → CLE6 loops γ1, γ2, . . .

uniform topology

slide-51
SLIDE 51

Thm [Bernardi, Holden, Sun]: Let (Mn, σn) uniformly random percolated triangulation of size n (n interior vertices, √n exterior vertices). There exist embeddings φn : Mn → D (and coupling) such that the following converge jointly in probability:

  • Area measure: vertex counting measure −

  • 8/3-LQG µ.
  • Exploration tree: τn → Branching SLE6 τ.
  • Percolation cycles:

embedded percolation cycles γn

1 , γn 2 , . . .

− → CLE6 loops γ1, γ2, . . .

uniform topology on subtrees

slide-52
SLIDE 52

Thm [Bernardi, Holden, Sun]: Let (Mn, σn) uniformly random percolated triangulation of size n (n interior vertices, √n exterior vertices). There exist embeddings φn : Mn → D (and coupling) such that the following converge jointly in probability:

  • Area measure: vertex counting measure −

  • 8/3-LQG µ.
  • Exploration tree: τn → Branching SLE6 τ.
  • Percolation cycles:

embedded percolation cycles γn

1 , γn 2 , . . .

− → CLE6 loops γ1, γ2, . . .

  • Pivotal measures: ∀ǫ, i, j, νǫ

i,n −

→ νǫ

i , and , νi,j,n−

→ νǫ

i,j.

weak topology

slide-53
SLIDE 53

Thm [Bernardi, Holden, Sun]: Let (Mn, σn) uniformly random percolated triangulation of size n (n interior vertices, √n exterior vertices). There exist embeddings φn : Mn → D (and coupling) such that the following converge jointly in probability:

  • Area measure: vertex counting measure −

  • 8/3-LQG µ.
  • Exploration tree: τn → Branching SLE6 τ.
  • Percolation cycles:

embedded percolation cycles γn

1 , γn 2 , . . .

− → CLE6 loops γ1, γ2, . . .

  • Crossing events: For random inner/outer vertex vn,

Eb(vn) − → Eb(v).

  • Pivotal measures: ∀ǫ, i, j, νǫ

i,n −

→ νǫ

i , and , νi,j,n−

→ νǫ

i,j.

slide-54
SLIDE 54

Strategy of proof:

Convergence of walk ++++ (Mn, σn) LQG√

8/3 + CLE6

slide-55
SLIDE 55

Strategy of proof:

Convergence of walk ++++

bijection

[Bernardi 2007] σ-algebra preserving coupling [Bernardi, Holden, Sun 2018] (Mn, σn) Zn Z LQG√

8/3 + CLE6

[Duplantier, Miller, Sheffield 2014] “mating of trees”

slide-56
SLIDE 56

Strategy of proof:

Convergence of walk ++++

bijection

Embedding φn defined using ”space filling exploration” [Bernardi 2007] σ-algebra preserving coupling [Bernardi, Holden, Sun 2018] (Mn, σn) Zn Z LQG√

8/3 + CLE6

[Duplantier, Miller, Sheffield 2014] “mating of trees”

slide-57
SLIDE 57

The bijection

slide-58
SLIDE 58

Kreweras walks Def. A Kreweras walk is a lattice walk on Z2 using the steps a = (1, 0), b = (0, 1) and c = (−1, −1). b a c

slide-59
SLIDE 59
  • Thm. There is a bijection between:
  • K = set of Kreweras walks starting and ending at (0, 0)

and staying in N2.

  • T = set of percolated triangulations of the disk

with 2 exterior vertices: one white and one black.

slide-60
SLIDE 60
  • Thm. There is a bijection between:
  • K = set of Kreweras walks starting and ending at (0, 0)

and staying in N2.

  • T = set of percolated triangulations of the disk

with 2 exterior vertices: one white and one black.

Φ

n interior vertices

K T

3n steps

slide-61
SLIDE 61
  • Thm. There is a bijection between:
  • K = set of Kreweras walks starting and ending at (0, 0)

and staying in N2.

  • T = set of percolated triangulations of the disk

with 2 exterior vertices: one white and one black.

Φ

n interior vertices

K T

3n steps 2n · 2n (n + 1)(2n + 1) 3n n

  • 4n

(n + 1)(2n + 1) 3n n

  • [Mullin 1965]

[Kreweras 1965]

slide-62
SLIDE 62

Example: w = baabbcacc

b a c

Φ

slide-63
SLIDE 63

Example: w = baabbcacc a a b b c a c c b

slide-64
SLIDE 64

Example: w = baabbcacc b a a b b b Definition:

b a

slide-65
SLIDE 65

Example: w = baabbcacc Definition:

c

c a c c

slide-66
SLIDE 66

a b c Well defined? #a − #c #b − #c

slide-67
SLIDE 67

a b c Well defined? #a − #c #b − #c Bijective? a a b b c a c c b

slide-68
SLIDE 68

a b c Well defined? #a − #c #b − #c a a b b c a c c b Bijective? reverse bijection

slide-69
SLIDE 69

Variants of the bijection Spherical case Disk case UIPT case

slide-70
SLIDE 70

Dictionary triangulation walk edges steps vertices c-steps black vertices c steps of type abc left-boundary length x-coordinate of walk walk perco-interface toward v walk of excursions clusters envelope intervals cluster’s bubbles cone intervals

slide-71
SLIDE 71

Dictionary triangulation walk edges steps vertices c-steps black vertices c steps of type abc left-boundary length x-coordinate of walk walk perco-interface toward v walk of excursions clusters envelope intervals cluster’s bubbles cone intervals

slide-72
SLIDE 72

Dictionary: percolation-interface to v ← → walk of excursions

slide-73
SLIDE 73

Dictionary: percolation-interface to v ← → walk of excursions Flatten each sub-excursion into a single step empty the bubbles Shuffle of 2 looptrees Flattened walk

slide-74
SLIDE 74

Dictionary: percolation-interface to v ← → walk of excursions

slide-75
SLIDE 75

discrete dictionary

continuum dictionary

[Duplantier, Miller, Sheffield] [Bernardi, Holden, Sun]

Perfect correspondence!

slide-76
SLIDE 76

More convergence results

under nice embedding + Miller, Sheffield Holden, Sun + Albenque, Garban, Gwynne, Lawler, Li, Sepulveda

slide-77
SLIDE 77

Cardy embedding of triangulations Theorem: Convergence holds for the Cardy embedding (p•, p•, p•) Cardy embedding where p• = Pperco

slide-78
SLIDE 78

Key ingredient needed: “convergence componentwise” Same triangulation k independent percolations k Kreweras walks k Brownian motions Same LQG k independent CLE

slide-79
SLIDE 79

Why needed? To upgrade the “crossing event result” from an annealed result to a quenched result. This implies (...) that φn ≃ Cardy embedding. Why needed?

slide-80
SLIDE 80

Why needed? To upgrade the “crossing event result” from an annealed result to a quenched result. This implies (...) that φn ≃ Cardy embedding. Why needed? How is it proved?

  • LQG stay the same: prove the previous convergence is joint

with convergence in Gromov-Hausdorff-Prokhorov topology.

  • CLE are independent: prove CLE mixes fast (using pivotal

point result).

slide-81
SLIDE 81

Thanks.