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Introduction Topological group case Model theory

When do closed classes imply closedness?

(and more)

Tomasz Rzepecki

Uniwersytet Wrocławski

¸ Sirince, May 2016

(2)

Introduction Topological group case Model theory

General setup Problem Transitive case

General setup

G is a group,

X is a set on which G acts,

E is a G-invariant equivalence relation on X (i.e. x E y ⇐⇒ gx E gy , for all x , y , g).

[Usually, we want to have x E y =⇒ G · x = G · y .]

Possible constraints:

The action is continuous.

G is compact.

(G, X are type-definable.) Etc.

(3)

Introduction Topological group case Model theory

General setup Problem Transitive case

General setup

G is a group,

X is a set on which G acts,

E is a G-invariant equivalence relation on X (i.e. x E y ⇐⇒ gx E gy , for all x , y , g).

[Usually, we want to have x E y =⇒ G · x = G · y .]

Possible constraints:

The action is continuous.

G is compact.

(G, X are type-definable.) Etc.

(4)

Introduction Topological group case Model theory

General setup Problem Transitive case

Problem

Question

If G is a topological group acting continuously on X , under what conditions is it true that E has closed classes iff it is closed [iff X /E is somehow nice]?

Example

Consider G =R acting on X = R2by r · (a, b) = (a + rb, b), and let E be the orbit equivalence relation.

Classes of E are points on the line y = 0 and lines parallel to it.

The classes of E are closed, and the class space is easy to understand (it is almost Hausdorff), but E is not closed.

(5)

Introduction Topological group case Model theory

General setup Problem Transitive case

Problem

Question

If G is a topological group acting continuously on X , under what conditions is it true that E has closed classes iff it is closed [iff X /E is somehow nice]?

Example

Consider G =R acting on X = R2by r · (a, b) = (a + rb, b), and let E be the orbit equivalence relation.

Classes of E are points on the line y = 0 and lines parallel to it.

The classes of E are closed, and the class space is easy to understand (it is almost Hausdorff), but E is not closed.

(6)

Introduction Topological group case Model theory

General setup Problem Transitive case

Very simple remark

Remark

Suppose G is a topological group and H ≤ G. Then H is closed iff the relation EH of lying in the same left coset of H is closed.

Proof.

EH = {(g1,g2) |g1−1g2∈ H}, while H = {g ∈ G | g EHe}, so EH is the preimage of H by the (continuous) map

(g1,g2) 7→g1−1g2and H is the section of EH at e.

Remark

If E is invariant on X = G, then E = EH, where H = [e]E.

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Introduction Topological group case Model theory

General setup Problem Transitive case

Example

We want at the very least to have that G\X is nice. For arbitrary continuous actions, various pathologies are possible.

Example

Consider G =R acting on the flat torus R2/Z2by

r · (a, b) = (a + r , b + r α) for a fixed α /∈ Q, and let E be the orbit equivalence relation.

Then E does not have closed classes (they are all meagre and dense), and the quotient space has no nice structure (e.g. the topology is trivial).

For simplicity, we will restrict ourselves to compact groups (acting on compact spaces).

(8)

Introduction Topological group case Model theory

General setup Problem Transitive case

Example

We want at the very least to have that G\X is nice. For arbitrary continuous actions, various pathologies are possible.

Example

Consider G =R acting on the flat torus R2/Z2by

r · (a, b) = (a + r , b + r α) for a fixed α /∈ Q, and let E be the orbit equivalence relation.

Then E does not have closed classes (they are all meagre and dense), and the quotient space has no nice structure (e.g. the topology is trivial).

For simplicity, we will restrict ourselves to compact groups (acting on compact spaces).

(9)

Introduction Topological group case Model theory

General setup Problem Transitive case

Example

We want at the very least to have that G\X is nice. For arbitrary continuous actions, various pathologies are possible.

Example

Consider G =R acting on the flat torus R2/Z2by

r · (a, b) = (a + r , b + r α) for a fixed α /∈ Q, and let E be the orbit equivalence relation.

Then E does not have closed classes (they are all meagre and dense), and the quotient space has no nice structure (e.g. the topology is trivial).

For simplicity, we will restrict ourselves to compact groups (acting on compact spaces).

(10)

Introduction Topological group case Model theory

General setup Problem Transitive case

Simple remark

Remark

Suppose G, X are compact, G acts transitively and continuously on X and E is invariant.

Then if E has closed classes, it is closed (in X2).

Proof.

Fix x0∈ X , put H := StabG[x0]E (preimage of [x0]E via the orbit map ϕx0:g 7→ g · x0).

Then g1x0E g2x0iff g1H = g2H.

It follows that E = {(g1x0,g2x0) |g1EH g2}, i.e. E is the pushforward of EH via ϕx0, so it is closed by

compactness.

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Introduction Topological group case Model theory

General setup Problem Transitive case

Simple remark

Remark

Suppose G, X are compact, G acts transitively and continuously on X and E is invariant.

Then if E has closed classes, it is closed (in X2).

Proof.

Fix x0∈ X , put H := StabG[x0]E (preimage of [x0]E via the orbit map ϕx0:g 7→ g · x0).

Then g1x0E g2x0iff g1H = g2H.

It follows that E = {(g1x0,g2x0) |g1EH g2}, i.e. E is the pushforward of EH via ϕx0, so it is closed by

compactness.

(12)

Introduction Topological group case Model theory

General setup Problem Transitive case

Simple remark

Remark

Suppose G, X are compact, G acts transitively and continuously on X and E is invariant.

Then if E has closed classes, it is closed (in X2).

Proof.

Fix x0∈ X , put H := StabG[x0]E (preimage of [x0]E via the orbit map ϕx0:g 7→ g · x0).

Then g1x0E g2x0iff g1H = g2H.

It follows that E = {(g1x0,g2x0) |g1EH g2}, i.e. E is the pushforward of EH via ϕx0, so it is closed by

compactness.

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Introduction Topological group case Model theory

General setup Problem Transitive case

Simple remark

Remark

Suppose G, X are compact, G acts transitively and continuously on X and E is invariant.

Then if E has closed classes, it is closed (in X2).

Proof.

Fix x0∈ X , put H := StabG[x0]E (preimage of [x0]E via the orbit map ϕx0:g 7→ g · x0).

Then g1x0E g2x0iff g1H = g2H.

It follows that E = {(g1x0,g2x0) |g1EH g2}, i.e. E is the pushforward of EH via ϕx0, so it is closed by

compactness.

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Introduction Topological group case Model theory

General setup Problem Transitive case

Gluing orbits

Remark

If E is finer than the orbit equivalence relation of G, then E is invariant iff each E G·x is invariant.

If G-orbits are closed and E is as above, then E has closed classes iff each E G·x has closed classes.

In general, there is no reason for E to be closed even if all E G·x are closed.

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Introduction Topological group case Model theory

General setup Problem Transitive case

Gluing orbits

Remark

If E is finer than the orbit equivalence relation of G, then E is invariant iff each E G·x is invariant.

If G-orbits are closed and E is as above, then E has closed classes iff each E G·x has closed classes.

In general, there is no reason for E to be closed even if all E G·x are closed.

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Introduction Topological group case Model theory

General setup Problem Transitive case

Gluing orbits

Remark

If E is finer than the orbit equivalence relation of G, then E is invariant iff each E G·x is invariant.

If G-orbits are closed and E is as above, then E has closed classes iff each E G·x has closed classes.

In general, there is no reason for E to be closed even if all E G·x are closed.

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Introduction Topological group case Model theory

General setup Problem Transitive case

Simple counterexample

Example

Let G =Z/2Z act on X = G × {0, 1/n | n ∈ N} in the natural way.

Put (g, x ) E (h, y ) iff x = y and (g = h or x 6= 0).

E is invariant, its classes are closed, but it is not closed.

Remark

This shows that we cannot just extend the preceding remark to intransitive actions.

We need to impose some additional condition on consistency of E across G-orbits.

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Introduction Topological group case Model theory

General setup Problem Transitive case

Simple counterexample

Example

Let G =Z/2Z act on X = G × {0, 1/n | n ∈ N} in the natural way.

Put (g, x ) E (h, y ) iff x = y and (g = h or x 6= 0).

E is invariant, its classes are closed, but it is not closed.

Remark

This shows that we cannot just extend the preceding remark to intransitive actions.

We need to impose some additional condition on consistency of E across G-orbits.

(19)

Introduction Topological group case Model theory

General setup Problem Transitive case

Simple counterexample

Example

Let G =Z/2Z act on X = G × {0, 1/n | n ∈ N} in the natural way.

Put (g, x ) E (h, y ) iff x = y and (g = h or x 6= 0).

E is invariant, its classes are closed, but it is not closed.

Remark

This shows that we cannot just extend the preceding remark to intransitive actions.

We need to impose some additional condition on consistency of E across G-orbits.

(20)

Introduction Topological group case Model theory

General setup Problem Transitive case

Simple counterexample

Example

Let G =Z/2Z act on X = G × {0, 1/n | n ∈ N} in the natural way.

Put (g, x ) E (h, y ) iff x = y and (g = h or x 6= 0).

E is invariant, its classes are closed, but it is not closed.

Remark

This shows that we cannot just extend the preceding remark to intransitive actions.

We need to impose some additional condition on consistency of E across G-orbits.

(21)

Introduction Topological group case Model theory

Smoothness Miller’s theorem Orbital equivalence relations Weakly orbital equivalence relations

Smoothness

Suppose we have an equivalence relation E on a Polish (=separable completely metrisable) space X . We say that E or X /E is smooth (“classifiable by reals”) if we can attach, in a Borel way, a unique real number to each E -class.

Fact

Any Gδ(in particular, any closed) equivalence relation is smooth.

Example

If we consider the action ofZ on the circle S1by an irrational rotation, then S1/Z is not smooth.

(22)

Introduction Topological group case Model theory

Smoothness Miller’s theorem Orbital equivalence relations Weakly orbital equivalence relations

Smoothness

Suppose we have an equivalence relation E on a Polish (=separable completely metrisable) space X . We say that E or X /E is smooth (“classifiable by reals”) if we can attach, in a Borel way, a unique real number to each E -class.

Fact

Any Gδ(in particular,any closed) equivalence relation is smooth.

Example

If we consider the action ofZ on the circle S1by an irrational rotation, then S1/Z is not smooth.

(23)

Introduction Topological group case Model theory

Smoothness Miller’s theorem Orbital equivalence relations Weakly orbital equivalence relations

Smoothness

Suppose we have an equivalence relation E on a Polish (=separable completely metrisable) space X . We say that E or X /E is smooth (“classifiable by reals”) if we can attach, in a Borel way, a unique real number to each E -class.

Fact

Any Gδ(in particular, any closed) equivalence relation is smooth.

Example

If we consider the action ofZ on the circle S1by an irrational rotation, then S1/Z is not smooth.

(24)

Introduction Topological group case Model theory

Smoothness Miller’s theorem Orbital equivalence relations Weakly orbital equivalence relations

Non-smoothness

Example

If we consider the action ofZ on the circle S1by an irrational rotation, then S1/Z is not smooth.

Proof.

Suppose towards contradiction that S1/Z is smooth, and let f : S1→ R be the Borel function witnessing that.

Then f is Baire measurable, so there is a comeagre set C ⊆ S1 such that f C is continuous.

Therefore, C0:=T

z∈Zz · C is also comeagre andZ-invariant, so it contains more than one orbit (because orbits are meagre).

But orbits are dense and f is constant on each of them, which is a contradiction, as f is continuous on C0.

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Introduction Topological group case Model theory

Smoothness Miller’s theorem Orbital equivalence relations Weakly orbital equivalence relations

Non-smoothness

Example

If we consider the action ofZ on the circle S1by an irrational rotation, then S1/Z is not smooth.

Proof.

Suppose towards contradiction that S1/Z is smooth, and let f : S1→ R be the Borel function witnessing that.

Then f is Baire measurable, so there is a comeagre set C ⊆ S1 such that f C is continuous.

Therefore, C0:=T

z∈Zz · C is also comeagre andZ-invariant, so it contains more than one orbit (because orbits are meagre).

But orbits are dense and f is constant on each of them, which is a contradiction, as f is continuous on C0.

(26)

Introduction Topological group case Model theory

Smoothness Miller’s theorem Orbital equivalence relations Weakly orbital equivalence relations

Non-smoothness

Example

If we consider the action ofZ on the circle S1by an irrational rotation, then S1/Z is not smooth.

Proof.

Suppose towards contradiction that S1/Z is smooth, and let f : S1→ R be the Borel function witnessing that.

Then f is Baire measurable, so there is a comeagre set C ⊆ S1 such that f C is continuous.

Therefore, C0:=T

z∈Zz · C is also comeagre andZ-invariant, so it contains more than one orbit (because orbits are meagre).

But orbits are dense and f is constant on each of them, which is a contradiction, as f is continuous on C0.

(27)

Introduction Topological group case Model theory

Smoothness Miller’s theorem Orbital equivalence relations Weakly orbital equivalence relations

Non-smoothness

Example

If we consider the action ofZ on the circle S1by an irrational rotation, then S1/Z is not smooth.

Proof.

Suppose towards contradiction that S1/Z is smooth, and let f : S1→ R be the Borel function witnessing that.

Then f is Baire measurable, so there is a comeagre set C ⊆ S1 such that f C is continuous.

Therefore, C0:=T

z∈Zz · C is also comeagre andZ-invariant, so it contains more than one orbit (because orbits are meagre).

But orbits are dense and f is constant on each of them, which is a contradiction, as f is continuous on C0.

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Introduction Topological group case Model theory

Smoothness Miller’s theorem Orbital equivalence relations Weakly orbital equivalence relations

Miller’s theorem

Fact (Miller, 1977)

Suppose G is a Polish group acting on X = G and H ≤ G. If EH is smooth, then H is closed.

Corollary (solution for the “transitive” case)

If G is a compact Polish group, acting continuously and transitively on a Polish space X , TFAE for invariant E on X :

1 E is closed,

2 E has closed classes,

3 E is smooth.

(29)

Introduction Topological group case Model theory

Smoothness Miller’s theorem Orbital equivalence relations Weakly orbital equivalence relations

Miller’s theorem

Fact (Miller, 1977)

Suppose G is a Polish group acting on X = G and H ≤ G. If EH is smooth, then H is closed.

Corollary (solution for the “transitive” case)

If G is a compact Polish group, acting continuously and transitively on a Polish space X , TFAE for invariant E on X :

1 E is closed,

2 E has closed classes,

3 E is smooth.

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Introduction Topological group case Model theory

Smoothness Miller’s theorem Orbital equivalence relations Weakly orbital equivalence relations

Proof of the transitive case

Corollary (solution for the “transitive” case)

If G is a compact Polish group, acting continuously and transitively on a Polish space X , TFAE for invariant E on X :

1 E is closed,

2 E has closed classes,

3 E is smooth.

Proof.

Assume that E is smooth. Fix any x0∈ X and let

H := StabG[x0]E. Then EH is smooth, so H is closed, so EH is closed and so is E (as in the previous proof).

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Introduction Topological group case Model theory

Smoothness Miller’s theorem Orbital equivalence relations Weakly orbital equivalence relations

Proof of the transitive case

Corollary (solution for the “transitive” case)

If G is a compact Polish group, acting continuously and transitively on a Polish space X , TFAE for invariant E on X :

1 E is closed,

2 E has closed classes,

3 E is smooth.

Proof.

Assume that E is smooth. Fix any x0∈ X and let

H := StabG[x0]E. Then EH is smooth, so H is closed, so EH is closed and so is E (as in the previous proof).

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Introduction Topological group case Model theory

Smoothness Miller’s theorem Orbital equivalence relations Weakly orbital equivalence relations

Smoothness and closedness

Corollary (solution for the “transitive” case)

If G is a compact Polish group, acting continuously and transitively on a Polish space X , TFAE for invariant E on X :

1 E is closed,

2 E has closed classes,

3 E is smooth.

Example

Suppose E is a (nontrivial) rotation-invariant equivalence relation on S1. Then E is smooth exactly when E = Eθ, where z1Eθz2 ⇐⇒ z1/z2=ek θi for some integer k , where θ is a (fixed) rational multiple of π.

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Introduction Topological group case Model theory

Smoothness Miller’s theorem Orbital equivalence relations Weakly orbital equivalence relations

Idea

In the transitive case, we had E = ϕx0[EH].

In general, given E refining G-orbit equivalence, we have E =S

x ∈XE G·x.

If each G · x is closed, and if E is smooth, then so are all E G·x.

Then for compact [Polish] G, X we have:

E closed =⇒ [E smooth =⇒ E G·x all smooth =⇒ ]

=⇒ [x ]E all closed =⇒ EG·x all closed For the missing implication, we need to have a better description of E than E =S

x ∈XE G·x.

Intuitively, we want to have that the transition between

“stalks” E G·x is “continuous”.

(34)

Introduction Topological group case Model theory

Smoothness Miller’s theorem Orbital equivalence relations Weakly orbital equivalence relations

Idea

In the transitive case, we had E = ϕx0[EH].

In general, given E refining G-orbit equivalence, we have E =S

x ∈XE G·x.

If each G · x is closed, and if E is smooth, then so are all E G·x.

Then for compact [Polish] G, X we have:

E closed =⇒ [E smooth =⇒ E G·x all smooth =⇒ ]

=⇒ [x ]E all closed =⇒ EG·x all closed For the missing implication, we need to have a better description of E than E =S

x ∈XE G·x.

Intuitively, we want to have that the transition between

“stalks” E G·x is “continuous”.

(35)

Introduction Topological group case Model theory

Smoothness Miller’s theorem Orbital equivalence relations Weakly orbital equivalence relations

Idea

In the transitive case, we had E = ϕx0[EH].

In general, given E refining G-orbit equivalence, we have E =S

x ∈XE G·x.

If each G · x is closed, and if E is smooth, then so are all E G·x.

Then for compact [Polish] G, X we have:

E closed =⇒ [E smooth =⇒ E G·x all smooth =⇒ ]

=⇒ [x ]E all closed =⇒ EG·x all closed For the missing implication, we need to have a better description of E than E =S

x ∈XE G·x.

Intuitively, we want to have that the transition between

“stalks” E G·x is “continuous”.

(36)

Introduction Topological group case Model theory

Smoothness Miller’s theorem Orbital equivalence relations Weakly orbital equivalence relations

Idea

In the transitive case, we had E = ϕx0[EH].

In general, given E refining G-orbit equivalence, we have E =S

x ∈XE G·x.

If each G · x is closed, and if E is smooth, then so are all E G·x.

Then for compact [Polish] G, X we have:

E closed =⇒ [E smooth =⇒ E G·x all smooth =⇒ ]

=⇒ [x ]E all closed =⇒ EG·x all closed For the missing implication, we need to have a better description of E than E =S

x ∈XE G·x.

Intuitively, we want to have that the transition between

“stalks” E G·x is “continuous”.

(37)

Introduction Topological group case Model theory

Smoothness Miller’s theorem Orbital equivalence relations Weakly orbital equivalence relations

Idea

In the transitive case, we had E = ϕx0[EH].

In general, given E refining G-orbit equivalence, we have E =S

x ∈XE G·x.

If each G · x is closed, and if E is smooth, then so are all E G·x.

Then for compact [Polish] G, X we have:

E closed =⇒ [E smooth =⇒ E G·x all smooth =⇒ ]

=⇒ [x ]E all closed =⇒ EG·x all closed For the missing implication, we need to have a better description of E than E =S

x ∈XE G·x.

Intuitively, we want to have that the transition between

“stalks” E G·x is “continuous”.

(38)

Introduction Topological group case Model theory

Smoothness Miller’s theorem Orbital equivalence relations Weakly orbital equivalence relations

Idea

In the transitive case, we had E = ϕx0[EH].

In general, given E refining G-orbit equivalence, we have E =S

x ∈XE G·x.

If each G · x is closed, and if E is smooth, then so are all E G·x.

Then for compact [Polish] G, X we have:

E closed =⇒ [E smooth =⇒ E G·x all smooth =⇒ ]

=⇒ [x ]E all closed =⇒ EG·x all closed For the missing implication, we need to have a better description of E than E =S

x ∈XE G·x.

Intuitively, we want to have that the transition between

“stalks” E G·x is “continuous”.

(39)

Introduction Topological group case Model theory

Smoothness Miller’s theorem Orbital equivalence relations Weakly orbital equivalence relations

Orbital equivalence relations

Definition

(An invariant equivalence relation) E is orbital if there is some H ≤ G such that for all x , [x ]E =H · x .

Intuition: E is orbital if for some H, the relation E is the “uniform pushforward” of EH by all the orbit maps; note that:

E = [

x ∈X

E G·x = [

x ∈X

ϕx[EH]

Example

Suppose G = X and H ≤ G. Then EH is orbital iff H is normal.

(Because an orbital equivalence relation on G is the relation of lying in therightcoset of a subgroup of G, and EH is the relation of lying in the sameleftcoset.)

(40)

Introduction Topological group case Model theory

Smoothness Miller’s theorem Orbital equivalence relations Weakly orbital equivalence relations

Orbital equivalence relations

Definition

(An invariant equivalence relation) E is orbital if there is some H ≤ G such that for all x , [x ]E =H · x .

Intuition: E is orbital if for some H, the relation E is the “uniform pushforward” of EH by all the orbit maps; note that:

E = [

x ∈X

E G·x = [

x ∈X

ϕx[EH]

Example

Suppose G = X and H ≤ G. Then EH is orbital iff H is normal.

(Because an orbital equivalence relation on G is the relation of lying in therightcoset of a subgroup of G, and EH is the relation of lying in the sameleftcoset.)

(41)

Introduction Topological group case Model theory

Smoothness Miller’s theorem Orbital equivalence relations Weakly orbital equivalence relations

Orbital equivalence relations

Definition

(An invariant equivalence relation) E is orbital if there is some H ≤ G such that for all x , [x ]E =H · x .

Intuition: E is orbital if for some H, the relation E is the “uniform pushforward” of EH by all the orbit maps; note that:

E = [

x ∈X

E G·x = [

x ∈X

ϕx[EH]

Example

Suppose G = X and H ≤ G. Then EH is orbital iff H is normal.

(Because an orbital equivalence relation on G is the relation of lying in therightcoset of a subgroup of G, and EH is the relation of lying in the sameleftcoset.)

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Introduction Topological group case Model theory

Smoothness Miller’s theorem Orbital equivalence relations Weakly orbital equivalence relations

Orbital equivalence relations ctd.

Definition

(An invariant equivalence relation) E is orbital if there is some H ≤ G such that for all x , [x ]E =H · x .

Lemma

Suppose E is orbital. Then orbitality is witnessed by H =T

x ∈XStabG[x ]E. Proof.

Let H0 witness orbitality of E . Then for all x we have

H0· x = [x]E ⊆ [x]E – so H0 ≤ H. On the other hand, we have by definition H · x ⊆ [x ]E =H0· x – so H · x ⊆ [x]E ⊆ H · x.

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Introduction Topological group case Model theory

Smoothness Miller’s theorem Orbital equivalence relations Weakly orbital equivalence relations

Orbital equivalence relations ctd.

Definition

(An invariant equivalence relation) E is orbital if there is some H ≤ G such that for all x , [x ]E =H · x .

Lemma

Suppose E is orbital. Then orbitality is witnessed by H =T

x ∈XStabG[x ]E. Proof.

Let H0 witness orbitality of E . Then for all x we have

H0· x = [x]E ⊆ [x]E – so H0 ≤ H. On the other hand, we have by definition H · x ⊆ [x ]E =H0· x – so H · x ⊆ [x]E ⊆ H · x.

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Introduction Topological group case Model theory

Smoothness Miller’s theorem Orbital equivalence relations Weakly orbital equivalence relations

Orbital equivalence relations ctd.

Definition

(An invariant equivalence relation) E is orbital if there is some H ≤ G such that for all x , [x ]E =H · x .

Proposition

Suppose G and X are compact and E is orbital. Then E is closed iff all of its classes are closed.

Proof.

Let H witness orbitality of E ; then E = {(x , hx ) | h ∈ H, x ∈ X }, which is closed if H is closed in G. ButT

x ∈XStabG[x ]E is closed and it witnesses orbitality.

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Introduction Topological group case Model theory

Smoothness Miller’s theorem Orbital equivalence relations Weakly orbital equivalence relations

Orbital equivalence relations ctd.

Definition

(An invariant equivalence relation) E is orbital if there is some H ≤ G such that for all x , [x ]E =H · x .

Proposition

Suppose G and X are compact and E is orbital. Then E is closed iff all of its classes are closed.

Proof.

Let H witness orbitality of E ; then E = {(x , hx ) | h ∈ H, x ∈ X }, which is closed if H is closed in G. ButT

x ∈XStabG[x ]E is closed and it witnesses orbitality.

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Introduction Topological group case Model theory

Smoothness Miller’s theorem Orbital equivalence relations Weakly orbital equivalence relations

Smoothness for orbital equivalence relations

Proposition

Suppose G and X are compact and E is orbital. Then E is closed iff all of its classes are closed.

Corollary (solution for the “orbital” case)

If G and X are compact Polish, while E is orbital, TFAE:

1 E is closed,

2 E has closed classes,

3 E is smooth.

Proof.

If E is smooth, so are all the E G·x, the classes are closed by the transitive case.

(47)

Introduction Topological group case Model theory

Smoothness Miller’s theorem Orbital equivalence relations Weakly orbital equivalence relations

Smoothness for orbital equivalence relations

Proposition

Suppose G and X are compact and E is orbital. Then E is closed iff all of its classes are closed.

Corollary (solution for the “orbital” case)

If G and X are compact Polish, while E is orbital, TFAE:

1 E is closed,

2 E has closed classes,

3 E is smooth.

Proof.

If E is smooth, so are all the E G·x, the classes are closed by the transitive case.

(48)

Introduction Topological group case Model theory

Smoothness Miller’s theorem Orbital equivalence relations Weakly orbital equivalence relations

Smoothness for orbital equivalence relations

Corollary (solution for the “orbital” case)

If G and X are compact Polish, while E is orbital, TFAE:

1 E is closed,

2 E has closed classes,

3 E is smooth.

Example

Consider G = SO(2) acting on X = D2. The smooth orbital equivalence relations are exactly those induced by finite subgroups of G.

(49)

Introduction Topological group case Model theory

Smoothness Miller’s theorem Orbital equivalence relations Weakly orbital equivalence relations

Weakly orbital equivalence relations

The “transitive” and “orbital” cases can be generalised together in the form of “weakly orbital” equivalence relations.

They can be intuitively interpreted as the relations which are “non-uniform” but still somehow consistent

pushforwards of some EH via the orbit maps.

Naively: put E =S

x ∈Xϕx[EHx]for some Hx ≤ G. But this is trivial: just take Hx =StabG[x ]E! We need more control over Hx.

(50)

Introduction Topological group case Model theory

Smoothness Miller’s theorem Orbital equivalence relations Weakly orbital equivalence relations

Weakly orbital equivalence relations

The “transitive” and “orbital” cases can be generalised together in the form of “weakly orbital” equivalence relations.

They can be intuitively interpreted as the relations which are “non-uniform” but still somehow consistent

pushforwards of some EH via the orbit maps.

Naively: put E =S

x ∈Xϕx[EHx]for some Hx ≤ G. But this is trivial: just take Hx =StabG[x ]E! We need more control over Hx.

(51)

Introduction Topological group case Model theory

Smoothness Miller’s theorem Orbital equivalence relations Weakly orbital equivalence relations

Weakly orbital equivalence relations

The “transitive” and “orbital” cases can be generalised together in the form of “weakly orbital” equivalence relations.

They can be intuitively interpreted as the relations which are “non-uniform” but still somehow consistent

pushforwards of some EH via the orbit maps.

Naively: put E =S

x ∈Xϕx[EHx]for some Hx ≤ G. But this is trivial: just take Hx =StabG[x ]E! We need more control over Hx.

(52)

Introduction Topological group case Model theory

Smoothness Miller’s theorem Orbital equivalence relations Weakly orbital equivalence relations

General (?) solution to the problem

Proposition (solution for the “weakly orbital” case)

Suppose G, X are compact Polish, and E is weakly orbital. The following are equivalent:

1 E is closed,

2 E has closed classes,

3 E is smooth.

(Thedenotes an extra assumption of “continuity” of the

“non-uniform” pushforward.)

(53)

Introduction Topological group case Model theory

Invariant equivalence relations in model theory Smoothness for BIERs

Previous results and the extension Definable group actions

Invariant equivalence relations in model theory

We consider a monster model C of a fixed complete first order theory T (i.e. a structure satisfying certain axioms and very rich in automorphisms).

Definition

We say that a set in (a power of) C is invariant when it is Aut(C)-invariant.

Definition

An invariant equivalence relation on some X ⊆ C is bounded if

|X /E| ≤ 2|T |(BIER). (Intuitively, X /E does not depend on C, only T .)

(54)

Introduction Topological group case Model theory

Invariant equivalence relations in model theory Smoothness for BIERs

Previous results and the extension Definable group actions

Invariant equivalence relations in model theory

We consider a monster model C of a fixed complete first order theory T (i.e. a structure satisfying certain axioms and very rich in automorphisms).

Definition

We say that a set in (a power of) C is invariant when it is Aut(C)-invariant.

Definition

An invariant equivalence relation on some X ⊆ C is bounded if

|X /E| ≤ 2|T |(BIER). (Intuitively, X /E does not depend on C, only T .)

(55)

Introduction Topological group case Model theory

Invariant equivalence relations in model theory Smoothness for BIERs

Previous results and the extension Definable group actions

Invariant equivalence relations in model theory

We consider a monster model C of a fixed complete first order theory T (i.e. a structure satisfying certain axioms and very rich in automorphisms).

Definition

We say that a set in (a power of) C is invariant when it is Aut(C)-invariant.

Definition

An invariant equivalence relation on some X ⊆ C is bounded if

|X /E| ≤ 2|T |(BIER). (Intuitively, X /E does not depend on C, only T .)

(56)

Introduction Topological group case Model theory

Invariant equivalence relations in model theory Smoothness for BIERs

Previous results and the extension Definable group actions

Lascar equivalence, (type-)definability

Definition

On any invariant set X , there is a finest BIER on X , denoted by

L.

Definition

We say that a set X ⊆ C is definable or “pseudo-clopen” (with parameters a1, . . . ,an) if there is a formula ϕ(x , a1, . . . ,an)in the language of T such that

X = {b ∈ C | ϕ(b, a1, . . . ,an) is true}

Definition

We call a set [∅-]type-definable or “pseudo-closed” when it is the intersection of a small family of sets definable [without parameters].

Tomasz Rzepecki When do closed classes imply closedness?

(57)

Introduction Topological group case Model theory

Invariant equivalence relations in model theory Smoothness for BIERs

Previous results and the extension Definable group actions

Lascar equivalence, (type-)definability

Definition

On any invariant set X , there is a finest BIER on X , denoted by

L.

Definition

We say that a set X ⊆ C is definable or “pseudo-clopen” (with parameters a1, . . . ,an) if there is a formula ϕ(x , a1, . . . ,an)in the language of T such that

X = {b ∈ C | ϕ(b, a1, . . . ,an) is true}

Definition

We call a set [∅-]type-definable or “pseudo-closed” when it is the intersection of a small family of sets definable [without parameters].

(58)

Introduction Topological group case Model theory

Invariant equivalence relations in model theory Smoothness for BIERs

Previous results and the extension Definable group actions

Lascar equivalence, (type-)definability

Definition

On any invariant set X , there is a finest BIER on X , denoted by

L.

Definition

We say that a set X ⊆ C is definable or “pseudo-clopen” (with parameters a1, . . . ,an) if there is a formula ϕ(x , a1, . . . ,an)in the language of T such that

X = {b ∈ C | ϕ(b, a1, . . . ,an) is true}

Definition

We call a set [∅-]type-definable or “pseudo-closed” when it is the intersection of a small family of sets definable [without parameters].

Tomasz Rzepecki When do closed classes imply closedness?

(59)

Introduction Topological group case Model theory

Invariant equivalence relations in model theory Smoothness for BIERs

Previous results and the extension Definable group actions

Smoothness in model theory

The notion of smoothness has been adapted to model theory in the following form.

Definition

Suppose E is a BIER and T is countable. Then EM is the

“pushforward” of E to the space of types over a countable model M (=orbits of Aut(C/M)).

Definition

We say that E is smooth if EM is smooth for some (every) countable model M.

(60)

Introduction Topological group case Model theory

Invariant equivalence relations in model theory Smoothness for BIERs

Previous results and the extension Definable group actions

Smoothness in model theory

The notion of smoothness has been adapted to model theory in the following form.

Definition

Suppose E is a BIER and T is countable. Then EM is the

“pushforward” of E to the space of types over a countable model M (=orbits of Aut(C/M)).

Definition

We say that E is smooth if EM is smooth for some (every) countable model M.

(61)

Introduction Topological group case Model theory

Invariant equivalence relations in model theory Smoothness for BIERs

Previous results and the extension Definable group actions

Previous results

Fact (Newelski 2002)

If ≡Lis not type-definable on X , then |X / ≡L| ≥ 20

Conjecture (Krupi ´nski, Pillay, Solecki 2012)

If T is countable, then ≡Lon a ∅-type-definable set is smooth iff it is type-definable (“closed”).

(Type-definable ⇒ smooth is easy.) Fact (Kaplan, Miller, Simon 2013) The conjecture holds.

(62)

Introduction Topological group case Model theory

Invariant equivalence relations in model theory Smoothness for BIERs

Previous results and the extension Definable group actions

Previous results

Fact (Newelski 2002)

If ≡Lis not type-definable on X , then |X / ≡L| ≥ 20

Conjecture (Krupi ´nski, Pillay, Solecki 2012)

If T is countable, then ≡Lon a ∅-type-definable set is smooth iff it is type-definable (“closed”).

(Type-definable ⇒ smooth is easy.) Fact (Kaplan, Miller, Simon 2013) The conjecture holds.

(63)

Introduction Topological group case Model theory

Invariant equivalence relations in model theory Smoothness for BIERs

Previous results and the extension Definable group actions

Previous results

Fact (Newelski 2002)

If ≡Lis not type-definable on X , then |X / ≡L| ≥ 20

Conjecture (Krupi ´nski, Pillay, Solecki 2012)

If T is countable, then ≡Lon a ∅-type-definable set is smooth iff it is type-definable (“closed”).

(Type-definable ⇒ smooth is easy.) Fact (Kaplan, Miller, Simon 2013) The conjecture holds.

(64)

Introduction Topological group case Model theory

Invariant equivalence relations in model theory Smoothness for BIERs

Previous results and the extension Definable group actions

The ultimate result?

Fact (Krupi ´nski, Pillay, Rz. 2015)

If E is a BIER on some [α](i.e. an Aut(C)-orbit) and T is countable, then E is smooth iff it is type-definable.

Remark

This is not true if the domain of E is not a complete type (i.e. Aut(C) does not act transitively on it).

The reason is the same as in the topological case:

essentially, gluing together countably many pieces preserves smoothness, but not type-definability.

(65)

Introduction Topological group case Model theory

Invariant equivalence relations in model theory Smoothness for BIERs

Previous results and the extension Definable group actions

The ultimate result?

Fact (Krupi ´nski, Pillay, Rz. 2015)

If E is a BIER on some [α](i.e. an Aut(C)-orbit) and T is countable, then E is smooth iff it is type-definable.

Remark

This is not true if the domain of E is not a complete type (i.e. Aut(C) does not act transitively on it).

The reason is the same as in the topological case:

essentially, gluing together countably many pieces preserves smoothness, but not type-definability.

(66)

Introduction Topological group case Model theory

Invariant equivalence relations in model theory Smoothness for BIERs

Previous results and the extension Definable group actions

The ultimate result?

Fact (Krupi ´nski, Pillay, Rz. 2015)

If E is a BIER on some [α](i.e. an Aut(C)-orbit) and T is countable, then E is smooth iff it is type-definable.

Remark

This is not true if the domain of E is not a complete type (i.e. Aut(C) does not act transitively on it).

The reason is the same as in the topological case:

essentially, gluing together countably many pieces preserves smoothness, but not type-definability.

(67)

Introduction Topological group case Model theory

Invariant equivalence relations in model theory Smoothness for BIERs

Previous results and the extension Definable group actions

The ultimate result?

Fact (Krupi ´nski, Pillay, Rz. 2015)

If E is a BIER on some [α](i.e. an Aut(C)-orbit) and T is countable, then E is smooth iff it is type-definable.

Remark

The fact does hold more generally, for example, in case of

Lon any ∅-type-definable set.

Lis an orbital equivalence relation w.r.t. G = Aut(C) (and it has a nice “consistent” syntactic description).

Weak orbitality is a way to express the “consistency” of the gluing.

(68)

Introduction Topological group case Model theory

Invariant equivalence relations in model theory Smoothness for BIERs

Previous results and the extension Definable group actions

The ultimate result?

Fact (Krupi ´nski, Pillay, Rz. 2015)

If E is a BIER on some [α](i.e. an Aut(C)-orbit) and T is countable, then E is smooth iff it is type-definable.

Remark

The fact does hold more generally, for example, in case of

Lon any ∅-type-definable set.

Lis an orbital equivalence relation w.r.t. G = Aut(C) (and it has a nice “consistent” syntactic description).

Weak orbitality is a way to express the “consistency” of the gluing.

(69)

Introduction Topological group case Model theory

Invariant equivalence relations in model theory Smoothness for BIERs

Previous results and the extension Definable group actions

The ultimate result?

Fact (Krupi ´nski, Pillay, Rz. 2015)

If E is a BIER on some [α](i.e. an Aut(C)-orbit) and T is countable, then E is smooth iff it is type-definable.

Remark

The fact does hold more generally, for example, in case of

Lon any ∅-type-definable set.

Lis an orbital equivalence relation w.r.t. G = Aut(C) (and it has a nice “consistent” syntactic description).

Weak orbitality is a way to express the “consistency” of the gluing.

(70)

Introduction Topological group case Model theory

Invariant equivalence relations in model theory Smoothness for BIERs

Previous results and the extension Definable group actions

The ultimate result?

Fact (Krupi ´nski, Pillay, Rz. 2015)

If E is a BIER on some [α](i.e. an Aut(C)-orbit) and T is countable, then E is smooth iff it is type-definable.

Remark

The fact does hold more generally, for example, in case of

Lon any ∅-type-definable set.

Lis an orbital equivalence relation w.r.t. G = Aut(C) (and it has a nice “consistent” syntactic description).

Weak orbitality is a way to express the “consistency” of the gluing.

(71)

Introduction Topological group case Model theory

Invariant equivalence relations in model theory Smoothness for BIERs

Previous results and the extension Definable group actions

Theorem

Suppose E is a BIER (on a ∅-type-definable set), weakly orbital with respect to G = Aut(C), while T is countable. Then TFAE:

E is type-definable,

all E -classes are type-definable, E is smooth.

Idea of the proof.

Such E can be seen as a “regular pushforward” of an

equivalence relation on Gal(T ), which allows us to reduce to the case of transitive Aut(C)-actions, which is the content of the preceding fact.

(72)

Introduction Topological group case Model theory

Invariant equivalence relations in model theory Smoothness for BIERs

Previous results and the extension Definable group actions

Theorem

Suppose E is a BIER (on a ∅-type-definable set), weakly orbital with respect to G = Aut(C), while T is countable. Then TFAE:

E is type-definable,

all E -classes are type-definable, E is smooth.

Idea of the proof.

Such E can be seen as a “regular pushforward” of an

equivalence relation on Gal(T ), which allows us to reduce to the case of transitive Aut(C)-actions, which is the content of the preceding fact.

(73)

Introduction Topological group case Model theory

Invariant equivalence relations in model theory Smoothness for BIERs

Previous results and the extension Definable group actions

(Type-)definable group actions

If G and X are ∅-type-definable, as is the group action, while all E -classes are (setwise) G000-invariant, we can prove a similar result by essentially the same methods.

(Note: G000is the so-called connected component of G.) Theorem

Suppose G, X , E are as above, and E is weakly orbital. Then E is type-definable iff all its classes are type-definable.

(74)

Introduction Topological group case Model theory

Invariant equivalence relations in model theory Smoothness for BIERs

Previous results and the extension Definable group actions

(Type-)definable group actions

If G and X are ∅-type-definable, as is the group action, while all E -classes are (setwise) G000-invariant, we can prove a similar result by essentially the same methods.

(Note: G000is the so-called connected component of G.) Theorem

Suppose G, X , E are as above, and E is weakly orbital. Then E is type-definable iff all its classes are type-definable.

(75)

Introduction Topological group case Model theory

Invariant equivalence relations in model theory Smoothness for BIERs

Previous results and the extension Definable group actions

Definable group actions and smoothness

Fact (Krupi ´nski, Pillay, Rz. 2015)

Suppose G is ∅-definable, T is countable, and H ≤ G is invariant of bounded index. Then EH is smooth iff H is type-definable.

(Note that H is invariant of bounded index iff EHis a BIER.) Corollary

Suppose that T is countable, G and X are ∅-definable, as is the action. If E is a weakly orbital, G-invariant BIER on X , then E is smooth iff it is type-definable.

(76)

Introduction Topological group case Model theory

Invariant equivalence relations in model theory Smoothness for BIERs

Previous results and the extension Definable group actions

Definable group actions and smoothness

Fact (Krupi ´nski, Pillay, Rz. 2015)

Suppose G is ∅-definable, T is countable, and H ≤ G is invariant of bounded index. Then EH is smooth iff H is type-definable.

(Note that H is invariant of bounded index iff EHis a BIER.) Corollary

Suppose that T is countable, G and X are ∅-definable, as is the action. If E is a weakly orbital, G-invariant BIER on X , then E is smooth iff it is type-definable.

Cytaty

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