Equidistribution for groups of toral automorphisms J. Bourgain A. - - PowerPoint PPT Presentation

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Equidistribution for groups of toral automorphisms J. Bourgain A. - - PowerPoint PPT Presentation

Equidistribution for groups of toral automorphisms J. Bourgain A. Furman E. Lindenstrauss S. Mozes 1 Institute for Advanced Study 2 University of Illinois at Chicago 3 Princeton and Hebrew University in Jerusalem 4 Hebrew University in


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Equidistribution for groups of toral automorphisms

  • J. Bourgain
  • A. Furman
  • E. Lindenstrauss
  • S. Mozes

1Institute for Advanced Study 2University of Illinois at Chicago 3Princeton and Hebrew University in Jerusalem 4Hebrew University in Jerusalem

UIC, May 2010

1/17

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SLIDE 2

Basic dynamical questions

General goal

T : X → X homeomorphism of a compact space X Understand the distribution of x, Tx, . . . , T Nx as N → ∞.

2/17

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Basic dynamical questions

General goal

T : X → X homeomorphism of a compact space X Understand the distribution of x, Tx, . . . , T Nx as N → ∞.

Levels of understanding

◮ Equidistribution: ∀x ∈ X, ∃µx ∈ PT(X)

1 N

N−1

  • n=0

f (T nx) →

  • X

f (y) dµx(y) (f ∈ C(X))

2/17

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SLIDE 4

Basic dynamical questions

General goal

T : X → X homeomorphism of a compact space X Understand the distribution of x, Tx, . . . , T Nx as N → ∞.

Levels of understanding

◮ Equidistribution: ∀x ∈ X, ∃µx ∈ PT(X)

1 N

N−1

  • n=0

f (T nx) →

  • X

f (y) dµx(y) (f ∈ C(X))

◮ Invariant measures: PT(X) = {µ ∈ P(X) : T∗µ = µ}

2/17

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SLIDE 5

Basic dynamical questions

General goal

T : X → X homeomorphism of a compact space X Understand the distribution of x, Tx, . . . , T Nx as N → ∞.

Levels of understanding

◮ Equidistribution: ∀x ∈ X, ∃µx ∈ PT(X)

1 N

N−1

  • n=0

f (T nx) →

  • X

f (y) dµx(y) (f ∈ C(X))

◮ Invariant measures: PT(X) = {µ ∈ P(X) : T∗µ = µ} ◮ Closed Invariant sets

2/17

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SLIDE 6

Toral automorphisms

A ∈ SLd(Z) acts on Td = Rd/Zd by A : x + Zd → Ax + Zd

3/17

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SLIDE 7

Toral automorphisms

A ∈ SLd(Z) acts on Td = Rd/Zd by A : x + Zd → Ax + Zd

Standard Example

A =

  • 2

1 1 1

  • 3/17
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SLIDE 8

Toral automorphisms

A ∈ SLd(Z) acts on Td = Rd/Zd by A : x + Zd → Ax + Zd

Standard Example

A =

  • 2

1 1 1

  • Observation

Periodic points =

  • p1

q , . . . , pd q

  • + Zd : gcd(p1, . . . , pd, q) = 1
  • 3/17
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SLIDE 9

Toral automorphisms

A ∈ SLd(Z) acts on Td = Rd/Zd by A : x + Zd → Ax + Zd

Standard Example

A =

  • 2

1 1 1

  • Observation

Periodic points =

  • p1

q , . . . , pd q

  • + Zd : gcd(p1, . . . , pd, q) = 1
  • Single hyperbolic automorphism

1 Closed Invariant sets: of every Hausdorff dim [0, d]

3/17

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SLIDE 10

Toral automorphisms

A ∈ SLd(Z) acts on Td = Rd/Zd by A : x + Zd → Ax + Zd

Standard Example

A =

  • 2

1 1 1

  • Observation

Periodic points =

  • p1

q , . . . , pd q

  • + Zd : gcd(p1, . . . , pd, q) = 1
  • Single hyperbolic automorphism

1 Closed Invariant sets: of every Hausdorff dim [0, d] 2 Invariant measures: uncountably many distinct ergodic

3/17

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SLIDE 11

Toral automorphisms

A ∈ SLd(Z) acts on Td = Rd/Zd by A : x + Zd → Ax + Zd

Standard Example

A =

  • 2

1 1 1

  • Observation

Periodic points =

  • p1

q , . . . , pd q

  • + Zd : gcd(p1, . . . , pd, q) = 1
  • Single hyperbolic automorphism

1 Closed Invariant sets: of every Hausdorff dim [0, d] 2 Invariant measures: uncountably many distinct ergodic 3 Equidistribution: no chance !

3/17

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SLIDE 12

Abelian groups of toral automorphisms

Setup

”Non degenerate” Zk < SLd(Z) with 2 ≤ k ≤ d − 1

4/17

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Abelian groups of toral automorphisms

Setup

”Non degenerate” Zk < SLd(Z) with 2 ≤ k ≤ d − 1

Rigidity phenomena

4/17

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SLIDE 14

Abelian groups of toral automorphisms

Setup

”Non degenerate” Zk < SLd(Z) with 2 ≤ k ≤ d − 1

Rigidity phenomena

1 Closed Invariant sets: Finite (rational pts), Td

  • H. Furstenberg (77), D. Berend (84)

4/17

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SLIDE 15

Abelian groups of toral automorphisms

Setup

”Non degenerate” Zk < SLd(Z) with 2 ≤ k ≤ d − 1

Rigidity phenomena

1 Closed Invariant sets: Finite (rational pts), Td

  • H. Furstenberg (77), D. Berend (84)

2 Invariant measures:

◮ Conjecture: Atomic (rational pts) + Lebesgue 4/17

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SLIDE 16

Abelian groups of toral automorphisms

Setup

”Non degenerate” Zk < SLd(Z) with 2 ≤ k ≤ d − 1

Rigidity phenomena

1 Closed Invariant sets: Finite (rational pts), Td

  • H. Furstenberg (77), D. Berend (84)

2 Invariant measures:

◮ Conjecture: Atomic (rational pts) + Lebesgue ◮ Positive entropy (equivalently dimH(µ) > 0) understood by:

  • D. Rudolph, A. Katok, R. Spatzier, B. Host, B. Kalinin,
  • E. Lindenstrauss, M. Einsiedler, ...

4/17

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SLIDE 17

Abelian groups of toral automorphisms

Setup

”Non degenerate” Zk < SLd(Z) with 2 ≤ k ≤ d − 1

Rigidity phenomena

1 Closed Invariant sets: Finite (rational pts), Td

  • H. Furstenberg (77), D. Berend (84)

2 Invariant measures:

◮ Conjecture: Atomic (rational pts) + Lebesgue ◮ Positive entropy (equivalently dimH(µ) > 0) understood by:

  • D. Rudolph, A. Katok, R. Spatzier, B. Host, B. Kalinin,
  • E. Lindenstrauss, M. Einsiedler, ...

3 No equidistribution

4/17

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SLIDE 18

Large groups of toral automorphisms

Setup

Γ < SLd(Z) which is Zariski dense in SLd(R)

5/17

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SLIDE 19

Large groups of toral automorphisms

Setup

Γ < SLd(Z) which is Zariski dense in SLd(R)

What is equidistribution for Γ.x ?

5/17

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SLIDE 20

Large groups of toral automorphisms

Setup

Γ < SLd(Z) which is Zariski dense in SLd(R)

What is equidistribution for Γ.x ?

Fix a prob meas ν on Γ with Γ = supp(ν). Consider µn,x = ν∗n ∗ δx =

  • ν(gn) · · · ν(g1) · δgn···g1x.

5/17

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SLIDE 21

Large groups of toral automorphisms

Setup

Γ < SLd(Z) which is Zariski dense in SLd(R)

What is equidistribution for Γ.x ?

Fix a prob meas ν on Γ with Γ = supp(ν). Consider µn,x = ν∗n ∗ δx =

  • ν(gn) · · · ν(g1) · δgn···g1x.

Remark

Weak-* limits of

1 N

N−1

n=0 µn,x are ν-stationary measures

Pν(X) =

  • µ ∈ P(X) : µ = ν ∗ µ =
  • ν(g) · g∗µ
  • 5/17
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SLIDE 22

Large groups of toral automorphisms

Setup

Γ < SLd(Z) which is Zariski dense in SLd(R)

What is equidistribution for Γ.x ?

Fix a prob meas ν on Γ with Γ = supp(ν). Consider µn,x = ν∗n ∗ δx =

  • ν(gn) · · · ν(g1) · δgn···g1x.

Remark

Weak-* limits of

1 N

N−1

n=0 µn,x are ν-stationary measures

Pν(X) =

  • µ ∈ P(X) : µ = ν ∗ µ =
  • ν(g) · g∗µ
  • ◮ PΓ(X) ⊆ Pν(X) convex compact subsets of P(X)

5/17

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SLIDE 23

Large groups of toral automorphisms

Setup

Γ < SLd(Z) which is Zariski dense in SLd(R)

What is equidistribution for Γ.x ?

Fix a prob meas ν on Γ with Γ = supp(ν). Consider µn,x = ν∗n ∗ δx =

  • ν(gn) · · · ν(g1) · δgn···g1x.

Remark

Weak-* limits of

1 N

N−1

n=0 µn,x are ν-stationary measures

Pν(X) =

  • µ ∈ P(X) : µ = ν ∗ µ =
  • ν(g) · g∗µ
  • ◮ PΓ(X) ⊆ Pν(X) convex compact subsets of P(X)

◮ PΓ(X) = ∅ is possible for non-amenable Γ.

5/17

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SLIDE 24

Large groups of toral automorphisms

Setup

Γ < SLd(Z) which is Zariski dense in SLd(R)

What is equidistribution for Γ.x ?

Fix a prob meas ν on Γ with Γ = supp(ν). Consider µn,x = ν∗n ∗ δx =

  • ν(gn) · · · ν(g1) · δgn···g1x.

Remark

Weak-* limits of

1 N

N−1

n=0 µn,x are ν-stationary measures

Pν(X) =

  • µ ∈ P(X) : µ = ν ∗ µ =
  • ν(g) · g∗µ
  • ◮ PΓ(X) ⊆ Pν(X) convex compact subsets of P(X)

◮ PΓ(X) = ∅ is possible for non-amenable Γ. ◮ Pν(X) = ∅, any closed invariant set supports ν-stationary measures

5/17

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SLIDE 25

Overview of the results

Setup

Γ < SLd(Z) which is Z-dense, or more generally

6/17

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SLIDE 26

Overview of the results

Setup

Γ < SLd(Z) which is Z-dense, or more generally Γ strongly irreducible and Γ ∋proximal element

6/17

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SLIDE 27

Overview of the results

Setup

Γ < SLd(Z) which is Z-dense, or more generally Γ strongly irreducible and Γ ∋proximal element

Rigidity phenomena

1 Closed Γ-invariant sets = Finite (rational pts), Td

  • R. Muchnik (05), Y. Guivarc’h-A. Starkov (04)

6/17

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SLIDE 28

Overview of the results

Setup

Γ < SLd(Z) which is Z-dense, or more generally Γ strongly irreducible and Γ ∋proximal element

Rigidity phenomena

1 Closed Γ-invariant sets = Finite (rational pts), Td

  • R. Muchnik (05), Y. Guivarc’h-A. Starkov (04)

2 Γ-invariant measures = Atomic (rational pts) + Lebesgue

BFLM (07, 10), Y. Benoist-J.F. Quint (10)

6/17

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SLIDE 29

Overview of the results

Setup

Γ < SLd(Z) which is Z-dense, or more generally Γ strongly irreducible and Γ ∋proximal element

Rigidity phenomena

1 Closed Γ-invariant sets = Finite (rational pts), Td

  • R. Muchnik (05), Y. Guivarc’h-A. Starkov (04)

2 Γ-invariant measures = Atomic (rational pts) + Lebesgue

BFLM (07, 10), Y. Benoist-J.F. Quint (10)

3 ν-stationary measures = Γ-invariant = Atomic + Lebesgue

BLFM (07, 10), Y. Benoist-J.F. Quint (10)

6/17

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SLIDE 30

Overview of the results

Setup

Γ < SLd(Z) which is Z-dense, or more generally Γ strongly irreducible and Γ ∋proximal element

Rigidity phenomena

1 Closed Γ-invariant sets = Finite (rational pts), Td

  • R. Muchnik (05), Y. Guivarc’h-A. Starkov (04)

2 Γ-invariant measures = Atomic (rational pts) + Lebesgue

BFLM (07, 10), Y. Benoist-J.F. Quint (10)

3 ν-stationary measures = Γ-invariant = Atomic + Lebesgue

BLFM (07, 10), Y. Benoist-J.F. Quint (10)

4 Equidistribution (in fact, quantitative!)

BLFM (07, 10). [BFLM] Stationary measures and equidistribution for orbits of non-abelian semi-groups on the torus, JAMS to appear.

6/17

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SLIDE 31

The main result (BFLM)

Assume ν on SLd(Z) with Γ = supp(ν) str irr + prox elmt and

7/17

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The main result (BFLM)

Assume ν on SLd(Z) with Γ = supp(ν) str irr + prox elmt and ∃ǫ > 0

  • g ν(g)gǫ < ∞.

7/17

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SLIDE 33

The main result (BFLM)

Assume ν on SLd(Z) with Γ = supp(ν) str irr + prox elmt and ∃ǫ > 0

  • g ν(g)gǫ < ∞.

Theorem (BFLM)

1 If x ∈ Td is irrational then

µn,x = ν∗n ∗ δx → Leb

7/17

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SLIDE 34

The main result (BFLM)

Assume ν on SLd(Z) with Γ = supp(ν) str irr + prox elmt and ∃ǫ > 0

  • g ν(g)gǫ < ∞.

Theorem (BFLM)

1 If x ∈ Td is irrational then

µn,x = ν∗n ∗ δx → Leb

2 If x ∈ Td is M-Diophantine (x − p q > 1 qM ) then

7/17

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SLIDE 35

The main result (BFLM)

Assume ν on SLd(Z) with Γ = supp(ν) str irr + prox elmt and ∃ǫ > 0

  • g ν(g)gǫ < ∞.

Theorem (BFLM)

1 If x ∈ Td is irrational then

µn,x = ν∗n ∗ δx → Leb

2 If x ∈ Td is M-Diophantine (x − p q > 1 qM ) then

| µn,x(a)| < a · e−cn/M

7/17

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SLIDE 36

The main result (BFLM)

Assume ν on SLd(Z) with Γ = supp(ν) str irr + prox elmt and ∃ǫ > 0

  • g ν(g)gǫ < ∞.

Theorem (BFLM)

1 If x ∈ Td is irrational then

µn,x = ν∗n ∗ δx → Leb

2 If x ∈ Td is M-Diophantine (x − p q > 1 qM ) then

| µn,x(a)| < a · e−cn/M

3 If |

µn,x(a)| = t > 0 for some a ∈ Zd − {0} with n > C log(2a/t)

7/17

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SLIDE 37

The main result (BFLM)

Assume ν on SLd(Z) with Γ = supp(ν) str irr + prox elmt and ∃ǫ > 0

  • g ν(g)gǫ < ∞.

Theorem (BFLM)

1 If x ∈ Td is irrational then

µn,x = ν∗n ∗ δx → Leb

2 If x ∈ Td is M-Diophantine (x − p q > 1 qM ) then

| µn,x(a)| < a · e−cn/M

3 If |

µn,x(a)| = t > 0 for some a ∈ Zd − {0} with n > C log(2a/t) then x − p q < e−λn with q < 2a t C

◮ where c > 0, λ > 0, C depend only on ν, ◮

µ(a) =

  • Td e2πia,x dµ(x) for a ∈ Zd.

7/17

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SLIDE 38

”Baby case”

Theorem (M. Burger)

Let µ ∈ P(Td) be invariant under a finite index subgroup Γ < SLd(Z). Then µ is a convex combination of Leb and atomic on finite orbits.

8/17

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SLIDE 39

”Baby case”

Theorem (M. Burger)

Let µ ∈ P(Td) be invariant under a finite index subgroup Γ < SLd(Z). Then µ is a convex combination of Leb and atomic on finite orbits.

Proof

1

g∗µ(a) =

  • Td e2πia,gx dµ(x) =
  • Td e2πig tra,x dµ(x) =

µ(g tra)

8/17

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SLIDE 40

”Baby case”

Theorem (M. Burger)

Let µ ∈ P(Td) be invariant under a finite index subgroup Γ < SLd(Z). Then µ is a convex combination of Leb and atomic on finite orbits.

Proof

1

g∗µ(a) =

  • Td e2πia,gx dµ(x) =
  • Td e2πig tra,x dµ(x) =

µ(g tra)

2 Wiener’s Lemma: x∈Td |µ({x})|2 = lim 1 |Bn|

  • a∈Bn |

µ(a)|2

8/17

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SLIDE 41

”Baby case”

Theorem (M. Burger)

Let µ ∈ P(Td) be invariant under a finite index subgroup Γ < SLd(Z). Then µ is a convex combination of Leb and atomic on finite orbits.

Proof

1

g∗µ(a) =

  • Td e2πia,gx dµ(x) =
  • Td e2πig tra,x dµ(x) =

µ(g tra)

2 Wiener’s Lemma: x∈Td |µ({x})|2 = lim 1 |Bn|

  • a∈Bn |

µ(a)|2 Assume µ is Γ-invariant and µ = Leb.

◮ |

µ(a)| = t > 0 for some a ∈ Zd \ {0}

8/17

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SLIDE 42

”Baby case”

Theorem (M. Burger)

Let µ ∈ P(Td) be invariant under a finite index subgroup Γ < SLd(Z). Then µ is a convex combination of Leb and atomic on finite orbits.

Proof

1

g∗µ(a) =

  • Td e2πia,gx dµ(x) =
  • Td e2πig tra,x dµ(x) =

µ(g tra)

2 Wiener’s Lemma: x∈Td |µ({x})|2 = lim 1 |Bn|

  • a∈Bn |

µ(a)|2 Assume µ is Γ-invariant and µ = Leb.

◮ |

µ(a)| = t > 0 for some a ∈ Zd \ {0}

◮ |

µ(g tra)|2 = | µ(a)|2 = t2 (g ∈ Γ)

8/17

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SLIDE 43

”Baby case”

Theorem (M. Burger)

Let µ ∈ P(Td) be invariant under a finite index subgroup Γ < SLd(Z). Then µ is a convex combination of Leb and atomic on finite orbits.

Proof

1

g∗µ(a) =

  • Td e2πia,gx dµ(x) =
  • Td e2πig tra,x dµ(x) =

µ(g tra)

2 Wiener’s Lemma: x∈Td |µ({x})|2 = lim 1 |Bn|

  • a∈Bn |

µ(a)|2 Assume µ is Γ-invariant and µ = Leb.

◮ |

µ(a)| = t > 0 for some a ∈ Zd \ {0}

◮ |

µ(g tra)|2 = | µ(a)|2 = t2 (g ∈ Γ)

◮ Density(|

µ|2) ≥ t2 · Density(Γtr.a) > 0

8/17

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SLIDE 44

”Baby case”

Theorem (M. Burger)

Let µ ∈ P(Td) be invariant under a finite index subgroup Γ < SLd(Z). Then µ is a convex combination of Leb and atomic on finite orbits.

Proof

1

g∗µ(a) =

  • Td e2πia,gx dµ(x) =
  • Td e2πig tra,x dµ(x) =

µ(g tra)

2 Wiener’s Lemma: x∈Td |µ({x})|2 = lim 1 |Bn|

  • a∈Bn |

µ(a)|2 Assume µ is Γ-invariant and µ = Leb.

◮ |

µ(a)| = t > 0 for some a ∈ Zd \ {0}

◮ |

µ(g tra)|2 = | µ(a)|2 = t2 (g ∈ Γ)

◮ Density(|

µ|2) ≥ t2 · Density(Γtr.a) > 0

◮ ⇒

µ has atoms (by Wiener)

8/17

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SLIDE 45

”Baby case”

Theorem (M. Burger)

Let µ ∈ P(Td) be invariant under a finite index subgroup Γ < SLd(Z). Then µ is a convex combination of Leb and atomic on finite orbits.

Proof

1

g∗µ(a) =

  • Td e2πia,gx dµ(x) =
  • Td e2πig tra,x dµ(x) =

µ(g tra)

2 Wiener’s Lemma: x∈Td |µ({x})|2 = lim 1 |Bn|

  • a∈Bn |

µ(a)|2 Assume µ is Γ-invariant and µ = Leb.

◮ |

µ(a)| = t > 0 for some a ∈ Zd \ {0}

◮ |

µ(g tra)|2 = | µ(a)|2 = t2 (g ∈ Γ)

◮ Density(|

µ|2) ≥ t2 · Density(Γtr.a) > 0

◮ ⇒

µ has atoms (by Wiener)

◮ Atoms of a Γ-inv prob measure belong to finite orbits.

8/17

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SLIDE 46

First glance at the problem

Make the proof for the following effective

If µ = ν ∗ µ has | µ(a)| = t > 0 for some a ∈ Zd \ {0}. Then µ has atoms.

9/17

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SLIDE 47

First glance at the problem

Make the proof for the following effective

If µ = ν ∗ µ has | µ(a)| = t > 0 for some a ∈ Zd \ {0}. Then µ has atoms.

Difficulties

1 ˆ

µ is not constant on Γ-orbits

9/17

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SLIDE 48

First glance at the problem

Make the proof for the following effective

If µ = ν ∗ µ has | µ(a)| = t > 0 for some a ∈ Zd \ {0}. Then µ has atoms.

Difficulties

1 ˆ

µ is not constant on Γ-orbits

2 Γ-orbits on Zd have zero density

9/17

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SLIDE 49

First glance at the problem

Make the proof for the following effective

If µ = ν ∗ µ has | µ(a)| = t > 0 for some a ∈ Zd \ {0}. Then µ has atoms.

Difficulties

1 ˆ

µ is not constant on Γ-orbits

2 Γ-orbits on Zd have zero density

Overcoming the difficulties

1 µ = ν ∗ µ = · · · = ν∗n ∗ µ

  • µ(a) = ν∗n(g) ·

µ(g tra)

9/17

slide-50
SLIDE 50

First glance at the problem

Make the proof for the following effective

If µ = ν ∗ µ has | µ(a)| = t > 0 for some a ∈ Zd \ {0}. Then µ has atoms.

Difficulties

1 ˆ

µ is not constant on Γ-orbits

2 Γ-orbits on Zd have zero density

Overcoming the difficulties

1 µ = ν ∗ µ = · · · = ν∗n ∗ µ

  • µ(a) = ν∗n(g) ·

µ(g tra) So | µ(a)| > t ⇒ ν∗n g : | µ(g tra)| > 1

2t

  • > 1

2t

9/17

slide-51
SLIDE 51

First glance at the problem

Make the proof for the following effective

If µ = ν ∗ µ has | µ(a)| = t > 0 for some a ∈ Zd \ {0}. Then µ has atoms.

Difficulties

1 ˆ

µ is not constant on Γ-orbits

2 Γ-orbits on Zd have zero density

Overcoming the difficulties

1 µ = ν ∗ µ = · · · = ν∗n ∗ µ

  • µ(a) = ν∗n(g) ·

µ(g tra) So | µ(a)| > t ⇒ ν∗n g : | µ(g tra)| > 1

2t

  • > 1

2t 2 This is 99% of the work !

9/17

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SLIDE 52

General strategy

10/17

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SLIDE 53

General strategy

1 Density> 0 at scales N, M = N1−κ for As = {b ∈ Zd : |

µ(b)| > s} NM(Ac1(t) ∩ [−N, N]d) > c2(t) · N

M

d where NM(S) - minimal number of M-cubes needed to cover S

10/17

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SLIDE 54

General strategy

1 Density> 0 at scales N, M = N1−κ for As = {b ∈ Zd : |

µ(b)| > s} NM(Ac1(t) ∩ [−N, N]d) > c2(t) · N

M

d where NM(S) - minimal number of M-cubes needed to cover S N |S| = 12 NM(S) = 5

slide-55
SLIDE 55

General strategy

1 Density> 0 at scales N, M = N1−κ for As = {b ∈ Zd : |

µ(b)| > s} NM(Ac1(t) ∩ [−N, N]d) > c2(t) · N

M

d where NM(S) - minimal number of M-cubes needed to cover S N M |S| = 12 NM(S) = 5

10/17

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SLIDE 56

General strategy

1 Density> 0 at scales N, M = N1−κ for As = {b ∈ Zd : |

µ(b)| > s} NM(Ac1(t) ∩ [−N, N]d) > c2(t) · N

M

d

2 µ is granulated

11/17

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SLIDE 57

General strategy

1 Density> 0 at scales N, M = N1−κ for As = {b ∈ Zd : |

µ(b)| > s} NM(Ac1(t) ∩ [−N, N]d) > c2(t) · N

M

d

2 µ is granulated There is 1/M-separated set {x1, . . . , xMd} ⊂ Td

µ Md

i=1 Bxi, 1

N

  • > c3(t),

µ(Bxi,r) > r d(1−κ)

11/17

slide-58
SLIDE 58

General strategy

1 Density> 0 at scales N, M = N1−κ for As = {b ∈ Zd : |

µ(b)| > s} NM(Ac1(t) ∩ [−N, N]d) > c2(t) · N

M

d

2 µ is granulated There is 1/M-separated set {x1, . . . , xMd} ⊂ Td

µ Md

i=1 Bxi, 1

N

  • > c3(t),

µ(Bxi,r) > r d(1−κ)

3 From granulation to atoms at rational points:

◮ Positive µ-mass at very dense balls µ(By,ρ) > ρǫ 11/17

slide-59
SLIDE 59

General strategy

1 Density> 0 at scales N, M = N1−κ for As = {b ∈ Zd : |

µ(b)| > s} NM(Ac1(t) ∩ [−N, N]d) > c2(t) · N

M

d

2 µ is granulated There is 1/M-separated set {x1, . . . , xMd} ⊂ Td

µ Md

i=1 Bxi, 1

N

  • > c3(t),

µ(Bxi,r) > r d(1−κ)

3 From granulation to atoms at rational points:

◮ Positive µ-mass at very dense balls µ(By,ρ) > ρǫ ◮ Dense balls are attracted to rational points 11/17

slide-60
SLIDE 60

General strategy

1 Density> 0 at scales N, M = N1−κ for As = {b ∈ Zd : |

µ(b)| > s} NM(Ac1(t) ∩ [−N, N]d) > c2(t) · N

M

d

2 µ is granulated There is 1/M-separated set {x1, . . . , xMd} ⊂ Td

µ Md

i=1 Bxi, 1

N

  • > c3(t),

µ(Bxi,r) > r d(1−κ)

3 From granulation to atoms at rational points:

◮ Positive µ-mass at very dense balls µ(By,ρ) > ρǫ ◮ Dense balls are attracted to rational points ◮ Gravitational collapse 11/17

slide-61
SLIDE 61

Products of random matrices

G = KA+K: g = k′ diag[et1, . . . , etd] k k, k′ ∈ SO(d), t1 ≥ · · · ≥ td A

slide-62
SLIDE 62

Products of random matrices

G = KA+K: g = k′ diag[et1, . . . , etd] k k, k′ ∈ SO(d), t1 ≥ · · · ≥ td A k(A)

slide-63
SLIDE 63

Products of random matrices

G = KA+K: g = k′ diag[et1, . . . , etd] k k, k′ ∈ SO(d), t1 ≥ · · · ≥ td A k(A) ·et ·e−t

slide-64
SLIDE 64

Products of random matrices

G = KA+K: g = k′ diag[et1, . . . , etd] k k, k′ ∈ SO(d), t1 ≥ · · · ≥ td A k(A) ·et ·e−t ·et ·e−t et e−t

  • k(A)
slide-65
SLIDE 65

Products of random matrices

G = KA+K: g = k′ diag[et1, . . . , etd] k k, k′ ∈ SO(d), t1 ≥ · · · ≥ td A k(A) ·et ·e−t ·et ·e−t et e−t

  • k(A)

g(A) θ

12/17

slide-66
SLIDE 66

Products of random matrices

G = KA+K: g = k′ diag[et1, . . . , etd] k k, k′ ∈ SO(d), t1 ≥ · · · ≥ td A k(A) ·et ·e−t ·et ·e−t et e−t

  • k(A)

g(A) θ Furstenberg, Guivarc’h, Raugi, LaPage, Goldsheid-Margulis,...

12/17

slide-67
SLIDE 67

Products of random matrices

G = KA+K: g = k′ diag[et1, . . . , etd] k k, k′ ∈ SO(d), t1 ≥ · · · ≥ td A k(A) ·et ·e−t ·et ·e−t et e−t

  • k(A)

g(A) θ Furstenberg, Guivarc’h, Raugi, LaPage, Goldsheid-Margulis,...

◮ ν∗n

  • g = k′

e(λ±ǫ)n e(−λ±ǫ)n

  • k
  • > 1 − e−cn

12/17

slide-68
SLIDE 68

Products of random matrices

G = KA+K: g = k′ diag[et1, . . . , etd] k k, k′ ∈ SO(d), t1 ≥ · · · ≥ td A k(A) ·et ·e−t ·et ·e−t et e−t

  • k(A)

g(A) θ Furstenberg, Guivarc’h, Raugi, LaPage, Goldsheid-Margulis,...

◮ ν∗n

  • g = k′

e(λ±ǫ)n e(−λ±ǫ)n

  • k
  • > 1 − e−cn

◮ ν∗n{g | θg ∈ Bξ,r} < r γ

for e−cn < r

12/17

slide-69
SLIDE 69

Large scale dimension

13/17

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SLIDE 70

Large scale dimension

◮ Given |

µ(a0)| = t0 > 0

13/17

slide-71
SLIDE 71

Large scale dimension

◮ Given |

µ(a0)| = t0 > 0 As = {b ∈ Zd : | µ(b)| > s}

13/17

slide-72
SLIDE 72

Large scale dimension

◮ Given |

µ(a0)| = t0 > 0 As = {b ∈ Zd : | µ(b)| > s}

◮ Want to show

NM(Ac(t) ∩ B0,N) > ˜ c(t) N

M

d

13/17

slide-73
SLIDE 73

Large scale dimension

◮ Given |

µ(a0)| = t0 > 0 As = {b ∈ Zd : | µ(b)| > s}

◮ Want to show

NM(Ac(t) ∩ B0,N) > ˜ c(t) N

M

d Random walks + stationarity ν∗n{g : | µ(g tra0)| > 1

2t0} > 1 2t0

13/17

slide-74
SLIDE 74

Large scale dimension

◮ Given |

µ(a0)| = t0 > 0 As = {b ∈ Zd : | µ(b)| > s}

◮ Want to show

NM(Ac(t) ∩ B0,N) > ˜ c(t) N

M

d Random walks + stationarity ν∗n{g : | µ(g tra0)| > 1

2t0} > 1 2t0 ◮ gives α0 > 0

NM(Ac0(t0) ∩ B0,N) > ˜ c0(t) N

M

α0

13/17

slide-75
SLIDE 75

Large scale dimension

◮ Given |

µ(a0)| = t0 > 0 As = {b ∈ Zd : | µ(b)| > s}

◮ Want to show

NM(Ac(t) ∩ B0,N) > ˜ c(t) N

M

d Random walks + stationarity ν∗n{g : | µ(g tra0)| > 1

2t0} > 1 2t0 ◮ gives α0 > 0

NM(Ac0(t0) ∩ B0,N) > ˜ c0(t) N

M

α0 Need to improve the dimension α = α0 to α = d in steps αi → αi+1 NMi(Ati ∩ B0,Ni) > ˜ ci(t) Ni Mi αi

13/17

slide-76
SLIDE 76

Additive structure of Fourier coefficients

Lemma

1 |A|2

  • a,b∈A

µ(a − b) ≥

  • 1

|A|

  • a∈A

µ(a)

  • 2

14/17

slide-77
SLIDE 77

Additive structure of Fourier coefficients

Lemma

1 |A|2

  • a,b∈A

µ(a − b) ≥

  • 1

|A|

  • a∈A

µ(a)

  • 2

Proof.

1 |A|2

  • a,b∈A

µ(a − b) =

1 |A|2

  • a,b∈A
  • Td e2πia−b,x dµ(x)

=

  • Td
  • 1

|A|

  • a∈A e2πia,x

·

  • 1

|A|

  • b∈A e2πib,x
  • dµ(x)

14/17

slide-78
SLIDE 78

Additive structure of Fourier coefficients

Lemma

1 |A|2

  • a,b∈A

µ(a − b) ≥

  • 1

|A|

  • a∈A

µ(a)

  • 2

Proof.

1 |A|2

  • a,b∈A

µ(a − b) =

1 |A|2

  • a,b∈A
  • Td e2πia−b,x dµ(x)

=

  • Td
  • 1

|A|

  • a∈A e2πia,x

·

  • 1

|A|

  • b∈A e2πib,x
  • dµ(x)

=

  • Td
  • 1

|A|

  • a∈A e2πia,x
  • 2

dµ(x) ≥

  • Td

1 |A|

  • a∈A e2πia,x dµ(x)
  • 2

=

  • 1

|A|

  • a∈A

µ(a)

  • 2

14/17

slide-79
SLIDE 79

Bourgain’s Projection Theorem (informal)

15/17

slide-80
SLIDE 80

Bourgain’s Projection Theorem (informal)

A ⊂ Rd, dim(A) = α, Θ ⊂ Pd−1, dim(Θ) ≥ γ ∃θ ∈ Θ dim(πθ(A)) > α+δ

d

15/17

slide-81
SLIDE 81

Bourgain’s Projection Theorem (informal)

A ⊂ Rd, dim(A) = α, Θ ⊂ Pd−1, dim(Θ) ≥ γ ∃θ ∈ Θ dim(πθ(A)) > α+δ

d

Theorem (Bourgain)

∀β, γ > 0, ∃δ > 0 so that ∀α ∈ [β, d − β]

◮ η ∈ P(Pd−1) with η(Bξ,r) < r γ ◮ A ⊂ B0,1 with Nr(A) ≥ r −α ◮ A, η not too degenerate

Then for η-most θ ∈ Pd−1 s.t. Nr(πθ(A)) > r − α+δ

d

A θ πθ(A)

15/17

slide-82
SLIDE 82

Bourgain’s Projection Theorem (informal)

A ⊂ Rd, dim(A) = α, Θ ⊂ Pd−1, dim(Θ) ≥ γ ∃θ ∈ Θ dim(πθ(A)) > α+δ

d

Theorem (Bourgain)

∀β, γ > 0, ∃δ > 0 so that ∀α ∈ [β, d − β]

◮ η ∈ P(Pd−1) with η(Bξ,r) < r γ ◮ A ⊂ B0,1 with Nr(A) ≥ r −α ◮ A, η not too degenerate

Then for η-most θ ∈ Pd−1 s.t. Nr(πθ(A)) > r − α+δ

d

A θ πθ(A)

Theorem (Marstrand, Falconer)

dim A + dim η > d

  • ∃θ,

Leb(πθ(A)) > 0

15/17

slide-83
SLIDE 83

Bourgain’s Projection Theorem (informal)

A ⊂ Rd, dim(A) = α, Θ ⊂ Pd−1, dim(Θ) ≥ γ ∃θ ∈ Θ dim(πθ(A)) > α+δ

d

Theorem (Bourgain)

∀β, γ > 0, ∃δ > 0 so that ∀α ∈ [β, d − β]

◮ η ∈ P(Pd−1) with η(Bξ,r) < r γ ◮ A ⊂ B0,1 with Nr(A) ≥ r −α ◮ A, η not too degenerate

Then for η-most θ ∈ Pd−1 s.t. Nr(πθ(A)) > r − α+δ

d

A θ πθ(A)

Theorem (Marstrand, Falconer)

dim A + dim η > d

  • ∃θ,

Leb(πθ(A)) > 0 α + γ > d

  • ∃θ,

Nr(πθ(A)) > cr −1

15/17

slide-84
SLIDE 84

Amplifying the dimension

A = Ati ∩ B0,Ni dim = αi

slide-85
SLIDE 85

Amplifying the dimension

A = Ati ∩ B0,Ni dim = αi dim(g tr(A)) > α+δ

2

slide-86
SLIDE 86

Amplifying the dimension

A = Ati ∩ B0,Ni dim = αi dim(g tr(A)) > α+δ

2

dim(htr(A)) > αi+δ

2

slide-87
SLIDE 87

Amplifying the dimension

A = Ati ∩ B0,Ni dim = αi dim(g tr(A)) > α+δ

2

dim(htr(A)) > αi+δ

2

∃g, h : 1 |A|2

  • a,b

| µ(g tra − htrb)| ≥

  • g

ν(g) · 1 |A|

  • a
  • µ(g tra)
  • 2

16/17

slide-88
SLIDE 88

Amplifying the dimension

A = Ati ∩ B0,Ni dim = αi dim(g tr(A)) > α+δ

2

dim(htr(A)) > αi+δ

2

dim(Ai+1) = αi+1 > αi + δ ∃g, h : 1 |A|2

  • a,b

| µ(g tra − htrb)| ≥

  • g

ν(g) · 1 |A|

  • a
  • µ(g tra)
  • 2

16/17

slide-89
SLIDE 89

Self packing of dense balls

slide-90
SLIDE 90

Self packing of dense balls

slide-91
SLIDE 91

Self packing of dense balls

slide-92
SLIDE 92

Self packing of dense balls

17/17