SLIDE 1 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
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
SLIDE 3 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
f (T nx) →
f (y) dµx(y) (f ∈ C(X))
2/17
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
f (T nx) →
f (y) dµx(y) (f ∈ C(X))
◮ Invariant measures: PT(X) = {µ ∈ P(X) : T∗µ = µ}
2/17
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
f (T nx) →
f (y) dµx(y) (f ∈ C(X))
◮ Invariant measures: PT(X) = {µ ∈ P(X) : T∗µ = µ} ◮ Closed Invariant sets
2/17
SLIDE 6 Toral automorphisms
A ∈ SLd(Z) acts on Td = Rd/Zd by A : x + Zd → Ax + Zd
3/17
SLIDE 7 Toral automorphisms
A ∈ SLd(Z) acts on Td = Rd/Zd by A : x + Zd → Ax + Zd
Standard Example
A =
1 1 1
SLIDE 8 Toral automorphisms
A ∈ SLd(Z) acts on Td = Rd/Zd by A : x + Zd → Ax + Zd
Standard Example
A =
1 1 1
Periodic points =
q , . . . , pd q
- + Zd : gcd(p1, . . . , pd, q) = 1
- 3/17
SLIDE 9 Toral automorphisms
A ∈ SLd(Z) acts on Td = Rd/Zd by A : x + Zd → Ax + Zd
Standard Example
A =
1 1 1
Periodic points =
q , . . . , pd q
- + Zd : gcd(p1, . . . , pd, q) = 1
- Single hyperbolic automorphism
1 Closed Invariant sets: of every Hausdorff dim [0, d]
3/17
SLIDE 10 Toral automorphisms
A ∈ SLd(Z) acts on Td = Rd/Zd by A : x + Zd → Ax + Zd
Standard Example
A =
1 1 1
Periodic points =
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
SLIDE 11 Toral automorphisms
A ∈ SLd(Z) acts on Td = Rd/Zd by A : x + Zd → Ax + Zd
Standard Example
A =
1 1 1
Periodic points =
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
SLIDE 12 Abelian groups of toral automorphisms
Setup
”Non degenerate” Zk < SLd(Z) with 2 ≤ k ≤ d − 1
4/17
SLIDE 13 Abelian groups of toral automorphisms
Setup
”Non degenerate” Zk < SLd(Z) with 2 ≤ k ≤ d − 1
Rigidity phenomena
4/17
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
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
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
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
SLIDE 18 Large groups of toral automorphisms
Setup
Γ < SLd(Z) which is Zariski dense in SLd(R)
5/17
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
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
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
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
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
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
SLIDE 25 Overview of the results
Setup
Γ < SLd(Z) which is Z-dense, or more generally
6/17
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
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
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
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
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
SLIDE 31 The main result (BFLM)
Assume ν on SLd(Z) with Γ = supp(ν) str irr + prox elmt and
7/17
SLIDE 32 The main result (BFLM)
Assume ν on SLd(Z) with Γ = supp(ν) str irr + prox elmt and ∃ǫ > 0
7/17
SLIDE 33 The main result (BFLM)
Assume ν on SLd(Z) with Γ = supp(ν) str irr + prox elmt and ∃ǫ > 0
Theorem (BFLM)
1 If x ∈ Td is irrational then
µn,x = ν∗n ∗ δx → Leb
7/17
SLIDE 34 The main result (BFLM)
Assume ν on SLd(Z) with Γ = supp(ν) str irr + prox elmt and ∃ǫ > 0
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
SLIDE 35 The main result (BFLM)
Assume ν on SLd(Z) with Γ = supp(ν) str irr + prox elmt and ∃ǫ > 0
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
SLIDE 36 The main result (BFLM)
Assume ν on SLd(Z) with Γ = supp(ν) str irr + prox elmt and ∃ǫ > 0
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
SLIDE 37 The main result (BFLM)
Assume ν on SLd(Z) with Γ = supp(ν) str irr + prox elmt and ∃ǫ > 0
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
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
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
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|
µ(a)|2
8/17
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|
µ(a)|2 Assume µ is Γ-invariant and µ = Leb.
◮ |
µ(a)| = t > 0 for some a ∈ Zd \ {0}
8/17
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|
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
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|
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
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|
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
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|
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
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
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
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
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(g tra)
9/17
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(g tra) So | µ(a)| > t ⇒ ν∗n g : | µ(g tra)| > 1
2t
2t
9/17
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(g tra) So | µ(a)| > t ⇒ ν∗n g : | µ(g tra)| > 1
2t
2t 2 This is 99% of the work !
9/17
SLIDE 52 General strategy
10/17
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
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 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
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
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
µ(Bxi,r) > r d(1−κ)
11/17
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
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 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
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 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
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
Products of random matrices
G = KA+K: g = k′ diag[et1, . . . , etd] k k, k′ ∈ SO(d), t1 ≥ · · · ≥ td A
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
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 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
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
g(A) θ
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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
g(A) θ Furstenberg, Guivarc’h, Raugi, LaPage, Goldsheid-Margulis,...
12/17
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
g(A) θ Furstenberg, Guivarc’h, Raugi, LaPage, Goldsheid-Margulis,...
◮ ν∗n
e(λ±ǫ)n e(−λ±ǫ)n
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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
g(A) θ Furstenberg, Guivarc’h, Raugi, LaPage, Goldsheid-Margulis,...
◮ ν∗n
e(λ±ǫ)n e(−λ±ǫ)n
◮ ν∗n{g | θg ∈ Bξ,r} < r γ
for e−cn < r
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SLIDE 69 Large scale dimension
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SLIDE 70 Large scale dimension
◮ Given |
µ(a0)| = t0 > 0
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SLIDE 71 Large scale dimension
◮ Given |
µ(a0)| = t0 > 0 As = {b ∈ Zd : | µ(b)| > s}
13/17
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 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 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 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 Additive structure of Fourier coefficients
Lemma
1 |A|2
µ(a − b) ≥
|A|
µ(a)
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SLIDE 77 Additive structure of Fourier coefficients
Lemma
1 |A|2
µ(a − b) ≥
|A|
µ(a)
Proof.
1 |A|2
µ(a − b) =
1 |A|2
=
|A|
·
|A|
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SLIDE 78 Additive structure of Fourier coefficients
Lemma
1 |A|2
µ(a − b) ≥
|A|
µ(a)
Proof.
1 |A|2
µ(a − b) =
1 |A|2
=
|A|
·
|A|
=
|A|
dµ(x) ≥
1 |A|
=
|A|
µ(a)
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SLIDE 79 Bourgain’s Projection Theorem (informal)
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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
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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)
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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
Leb(πθ(A)) > 0
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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
Leb(πθ(A)) > 0 α + γ > d
Nr(πθ(A)) > cr −1
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SLIDE 84
Amplifying the dimension
A = Ati ∩ B0,Ni dim = αi
SLIDE 85 Amplifying the dimension
A = Ati ∩ B0,Ni dim = αi dim(g tr(A)) > α+δ
2
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 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
| µ(g tra − htrb)| ≥
ν(g) · 1 |A|
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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
| µ(g tra − htrb)| ≥
ν(g) · 1 |A|
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SLIDE 89
Self packing of dense balls
SLIDE 90
Self packing of dense balls
SLIDE 91
Self packing of dense balls
SLIDE 92 Self packing of dense balls
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