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Smoothness of bounded invariant equivalence relations

Tomasz Rzepecki

(joint work with Krzysztof Krupi ´nski)

Uniwersytet Wrocławski

Classification Theory Workshop, 2014

(2)

Motivations

General goal: understanding “strong type spaces”.

A theorem of Newelski (2002) about Fσ equivalence relations (cardinality).

A theorem of Kaplan, Miller and Simon (2013) about Borel cardinality of Lascar strong type (Borel cardinality).

A question of Gismatullin and Krupi ´nski (2012) related to connected group components.

(3)

Motivations

General goal: understanding “strong type spaces”.

A theorem of Newelski (2002) about Fσ equivalence relations (cardinality).

A theorem of Kaplan, Miller and Simon (2013) about Borel cardinality of Lascar strong type (Borel cardinality).

A question of Gismatullin and Krupi ´nski (2012) related to connected group components.

(4)

Motivations

General goal: understanding “strong type spaces”.

A theorem of Newelski (2002) about Fσ equivalence relations (cardinality).

A theorem of Kaplan, Miller and Simon (2013) about Borel cardinality of Lascar strong type (Borel cardinality).

A question of Gismatullin and Krupi ´nski (2012) related to connected group components.

(5)

Motivations

General goal: understanding “strong type spaces”.

A theorem of Newelski (2002) about Fσ equivalence relations (cardinality).

A theorem of Kaplan, Miller and Simon (2013) about Borel cardinality of Lascar strong type (Borel cardinality).

A question of Gismatullin and Krupi ´nski (2012) related to connected group components.

(6)

Borel reductions

Definition

Suppose X , Y are Polish spaces and E , F are Borel equivalence relations on X , Y . Then f : X → Y is aBorel reductionof E to F if

f (x ) F f (x0) ⇐⇒ x E x0

(7)

Borel cardinalities

1= (1) (2)

(N) (3) (R) E0

(n)

smooth

Definition

E ≤BF if there exists a Borel reduction of E to F . E ∼BF if E ≤B F and F ≤BE ; E

is smooth if E ∼B∆(X ).

Fact

There is a smallest non-smooth equivalence relation,E0.

B is linear up toE0.

(8)

Borel cardinalities

1= (1) (2)

(N) (3) (R) E0

(n)

smooth

Definition

E ≤BF if there exists a Borel reduction of E to F . E ∼BF if E ≤B F and F ≤BE ; E

is smooth if E ∼B∆(X ).

Fact

There is a smallest non-smooth equivalence relation,E0.

B is linear up toE0.

(9)

Strong types

≡KP ≡L

Definition

KP is the finest bounded (i.e. with small number of classes), ∅-type-definable equivalence relation.

L is the finest bounded, invariant equivalence relation.

Fact

Lis (∅−)Fσ, i.e. x ≡Ly ⇐⇒ W

nΦn(x , y ).

In the sequel, E is a bounded, Fσ equivalence

(10)

Strong types

≡KP ≡L

Definition

KP is the finest bounded (i.e. with small number of classes), ∅-type-definable equivalence relation.

L is the finest bounded, invariant equivalence relation.

Fact

Lis (∅−)Fσ, i.e. x ≡Ly ⇐⇒ W

nΦn(x , y ).

In the sequel, E is a bounded, Fσ equivalence

(11)

Strong types

≡KP ≡L

Definition

KP is the finest bounded (i.e. with small number of classes), ∅-type-definable equivalence relation.

L is the finest bounded, invariant equivalence relation.

Fact

Lis (∅−)Fσ, i.e. x ≡Ly ⇐⇒ W

nΦn(x , y ).

In the sequel, E is a bounded, Fσ equivalence

(12)

Borel cardinalities of invariant equivalence relations

SX(M) EM

S(M) E

X

Definition

Borel cardinality of E is the Borel cardinality of EM for a ctble model M.

p EM q ⇐⇒ ∃a |= p ∃b |= q (a E b)

Remark

Type-definable ERs (e.g. ≡KP) are smooth.

(13)

Borel cardinalities of invariant equivalence relations

SX(M) EM

S(M) E

X

Definition

Borel cardinality of E is the Borel cardinality of EM for a ctble model M.

p EM q ⇐⇒ ∃a |= p ∃b |= q (a E b)

Remark

Type-definable ERs (e.g. ≡KP) are smooth.

(14)

Orbital equivalence relations

Definition

As before, E is an Fσ, bounded equivalence relation on X ⊆ C.

E is orbital if there is some Γ ≤ Aut(C) such that E -classes are orbits of Γ.

E is orbital on types if it refines ≡ and restrictions of E to types are orbital.

Example

KP and ≡Lare orbital.

(15)

Orbital equivalence relations

Definition

As before, E is an Fσ, bounded equivalence relation on X ⊆ C.

E is orbital if there is some Γ ≤ Aut(C) such that E -classes are orbits of Γ.

E is orbital on types if it refines ≡ and restrictions of E to types are orbital.

Example

KP and ≡Lare orbital.

(16)

Orbital on types vs refining ≡

Question

If E refines ≡, is E already orbital on types?

Answer

No! (We have found counterexamples.)

(17)

Normal form

Definition

If E is Fσ on X , thenW

nΦn(x , y ) is a normal form for E if it is increasing (i.e. Φn` Φn+1),

E (x , y ) ⇐⇒ W

nΦn(x , y ),

d (x , y ) = min{n | C |= Φn(x , y )} is a metric on X .

Example

Lis has normal form Φn(x , y ) = “dL(x , y ) ≤ n” (Lascar distance).

(18)

Normal form

Definition

If E is Fσ on X , thenW

nΦn(x , y ) is a normal form for E if it is increasing (i.e. Φn` Φn+1),

E (x , y ) ⇐⇒ W

nΦn(x , y ),

d (x , y ) = min{n | C |= Φn(x , y )} is a metric on X .

Example

Lis has normal form Φn(x , y ) = “dL(x , y ) ≤ n” (Lascar distance).

(19)

Normal form

Definition

If E is Fσ on X , thenW

nΦn(x , y ) is a normal form for E if it is increasing (i.e. Φn` Φn+1),

E (x , y ) ⇐⇒ W

nΦn(x , y ),

d (x , y ) = min{n | C |= Φn(x , y )} is a metric on X .

Example

Lis has normal form Φn(x , y ) = “dL(x , y ) ≤ n” (Lascar distance).

(20)

Normal form

Definition

If E is Fσ on X , thenW

nΦn(x , y ) is a normal form for E if it is increasing (i.e. Φn` Φn+1),

E (x , y ) ⇐⇒ W

nΦn(x , y ),

d (x , y ) = min{n | C |= Φn(x , y )} is a metric on X .

Example

Lis has normal form Φn(x , y ) = “dL(x , y ) ≤ n” (Lascar distance).

(21)

Normal forms exist

Proposition

If E is bounded Fσ, then E has a normal formW

nΦnsuch that

“dL(x , y ) ≤ n” ` Φn(x , y ).

Proposition

C: an E -class;assume that E refines ≡. TFAE:

C has infinite diameter w.r.t. somenormal form;

C has infinite diameter w.r.t. everynormal form.

Proof.

Easy from a theorem of Newelski.

(22)

Normal forms exist

Proposition

If E is bounded Fσ, then E has a normal formW

nΦnsuch that

“dL(x , y ) ≤ n” ` Φn(x , y ).

Proposition

C: an E -class;assume that E refines ≡. TFAE:

C has infinite diameter w.r.t. somenormal form;

C has infinite diameter w.r.t. everynormal form.

Proof.

Easy from a theorem of Newelski.

(23)

Normal forms exist

Proposition

If E is bounded Fσ, then E has a normal formW

nΦnsuch that

“dL(x , y ) ≤ n” ` Φn(x , y ).

Proposition

C: an E -class;assume that E refines ≡. TFAE:

C has infinite diameter w.r.t. somenormal form;

C has infinite diameter w.r.t. everynormal form.

Proof.

Easy from a theorem of Newelski.

(24)

Technical theorem

Fact (Newelski 2002, simplified) E : Fσ, refines ≡.

Then if [a]E has infinite diameter, then E [a]has at least c classes.

Fact (Kaplan, Miller & Simon 2013)

The class [a]L has infinite diameter (w.r.t. Lascar distance) iff

L[a]is non-smooth.

Theorem (countable case; independently Kaplan & Miller 2013) E : is bdd, Fσ andorbital on types.

(25)

Technical theorem

Fact (Newelski 2002, simplified) E : Fσ, refines ≡.

Then if [a]E has infinite diameter, then E [a]has at least c classes.

Fact (Kaplan, Miller & Simon 2013)

The class [a]L has infinite diameter (w.r.t. Lascar distance) iff

L[a]is non-smooth.

Theorem (countable case; independently Kaplan & Miller 2013) E : is bdd, Fσ andorbital on types.

(26)

Technical theorem

Fact (Newelski 2002, simplified) E : Fσ, refines ≡.

Then if [a]E has infinite diameter, then E [a]has at least c classes.

Fact (Kaplan, Miller & Simon 2013)

The class [a]L has infinite diameter (w.r.t. Lascar distance) iff

L[a]is non-smooth.

Theorem (countable case; independently Kaplan & Miller 2013) E : is bdd, Fσ andorbital on types.

(27)

Technical theorem cont.

Corollary (countable case for groups)

G: definable and N E G: Fσ of bounded index.

Then N is ∅-type-definable ⇐⇒ ENis smooth.

Remark

Similar result in uncountable case, more complicated techniques.

(28)

Technical theorem cont.

Corollary (countable case for groups)

G: definable and N E G: Fσ of bounded index.

Then N is ∅-type-definable ⇐⇒ ENis smooth.

Remark

Similar result in uncountable case, more complicated techniques.

(29)

Five conditions theorem

Theorem

E : orbital on types, Fσ, bdd. ER on X : Bounded diameters

⇑ if X = p(C)













Type-definable

Smooth ⇔ finite diameters













⇑ if E ⊆ ≡KP

E is refined by ≡KP

(30)

Five conditions theorem

Theorem

E : orbital on types, Fσ, bdd. ER on X : Bounded diameters

⇑ if X = p(C)













Type-definable

Smooth ⇔ finite diameters













⇑ if E ⊆ ≡KP

E is refined by ≡KP

(31)

Five conditions theorem

Theorem

E : orbital on types, Fσ, bdd. ER on X : Bounded diameters

⇑ if X = p(C)













Type-definable

Smooth ⇔ finite diameters













⇑ if E ⊆ ≡KP

E is refined by ≡KP

(32)

Additional comments

Proposition

Reverse (⇑) implications do not hold.

Proof.

Series of counterexamples.

Question

Can we weaken “orbital on types” assumption?

Answer (partial)

Not too much: E must at least refine ≡.

(33)

Additional comments

Proposition

Reverse (⇑) implications do not hold.

Proof.

Series of counterexamples.

Question

Can we weaken “orbital on types” assumption?

Answer (partial)

Not too much: E must at least refine ≡.

(34)

Additional comments

Proposition

Reverse (⇑) implications do not hold.

Proof.

Series of counterexamples.

Question

Can we weaken “orbital on types” assumption?

Answer (partial)

Not too much: E must at least refine ≡.

(35)

Examples

1

3|(x- )

E

1

p

0

Example

T = Th(Z, +, n|·)n∈N; p0(x ) = tp(1/∅) =V

nn6 |x x E y ⇐⇒ x ≡ y and if x |= p0, then 3|(x − y ).

E :

issmooth, butnot type-definable, is orbital on types (so theorem applies).

(36)

Examples

1

3|(x- )

E

1

p

0

Example

T = Th(Z, +, n|·)n∈N; p0(x ) = tp(1/∅) =V

nn6 |x x E y ⇐⇒ x ≡ y and if x |= p0, then 3|(x − y ).

E :

issmooth, butnot type-definable, is orbital on types (so theorem applies).

(37)

Examples

1

3|(x- )

E

1

p

0

Example

T = Th(Z, +, n|·)n∈N; p0(x ) = tp(1/∅) =V

nn6 |x x E y ⇐⇒ x ≡ y and if x |= p0, then 3|(x − y ).

E :

issmooth, butnot type-definable, is orbital on types (so theorem applies).

(38)

Examples

1

3|(x- )

E

1

p

0

Example

T = Th(Z, +, n|·)n∈N; p0(x ) = tp(1/∅) =V

nn6 |x x E y ⇐⇒ x ≡ y and if x |= p0, then 3|(x − y ).

E :

issmooth, butnot type-definable, is orbital on types (so theorem applies).

(39)

Examples

1

3|(x- )

E

1

p

0

Example

T = Th(Z, +, n|·)n∈N; p0(x ) = tp(1/∅) =V

nn6 |x x E y ⇐⇒ x ≡ y and if x |= p0, then 3|(x − y ).

E :

issmooth, butnot type-definable, is orbital on types (so theorem applies).

(40)

Examples

...

...

...

...

...

Example

T = Th(R, +, ·, 1, 0, <);

Φn(x , y ) =V

m≥n(x < m ↔ y < m);

E =W

nΦn(x , y )

E has only 2 classes (so it issmooth), although one class hasinfinite diameter (and E is not type-definable).

E does not refine ≡ (theorem does not apply).

(41)

Examples

...

...

...

...

...

Example

T = Th(R, +, ·, 1, 0, <);

Φn(x , y ) =V

m≥n(x < m ↔ y < m);

E =W

nΦn(x , y )

E has only 2 classes (so it issmooth), although one class hasinfinite diameter (and E is not type-definable).

E does not refine ≡ (theorem does not apply).

(42)

Examples

...

...

...

...

...

Example

T = Th(R, +, ·, 1, 0, <);

Φn(x , y ) =V

m≥n(x < m ↔ y < m);

E =W

nΦn(x , y )

E has only 2 classes (so it issmooth), although one class hasinfinite diameter (and E is not type-definable).

E does not refine ≡ (theorem does not apply).

(43)

Examples

...

...

...

...

...

Example

T = Th(R, +, ·, 1, 0, <);

Φn(x , y ) =V

m≥n(x < m ↔ y < m);

E =W

nΦn(x , y )

E has only 2 classes (so it issmooth), although one class hasinfinite diameter (and E is not type-definable).

E does not refine ≡ (theorem does not apply).

(44)

Examples

...

...

...

...

...

Example

T = Th(R, +, ·, 1, 0, <);

Φn(x , y ) =V

m≥n(x < m ↔ y < m);

E =W

nΦn(x , y )

E has only 2 classes (so it issmooth), although one class hasinfinite diameter (and E is not type-definable).

E does not refine ≡ (theorem does not apply).

(45)

Connected components

Definition

G: (∅-) definable group in C.

G00 : the smallest type-definable subgroup of bounded index;

G000 : the smallest invariant subgroup of bounded index.

Question

Are there definable groups such that G00 6= G000?

Answer (Pillay & Conversano 2012)

(46)

Connected components

Definition

G: (∅-) definable group in C.

G00 : the smallest type-definable subgroup of bounded index;

G000 : the smallest invariant subgroup of bounded index.

Question

Are there definable groups such that G00 6= G000? Answer (Pillay & Conversano 2012)

(47)

Connected components

Definition

G: (∅-) definable group in C.

G00 : the smallest type-definable subgroup of bounded index;

G000 : the smallest invariant subgroup of bounded index.

Question

Are there definable groups such that G00 6= G000? Answer (Pillay & Conversano 2012)

(48)

Connected components: meta-example

Theorem (Gismatullin, Krupi ´nski 2012) 0 → A → eG→ G → 0π A, G: definable groups (A abelian),

G = A × G:e definable group in terms of 2-cocyle h : G2→ A.

Under some technical assumptions andassumption †

(concerning non-splitting of a cocycle derived from h), we have

Ge006= eG000.

(49)

Connected components: meta-example

Theorem (Gismatullin, Krupi ´nski 2012) 0 → A → eG→ G → 0π A, G: definable groups (A abelian),

G = A × G:e definable group in terms of 2-cocyle h : G2→ A.

Under some technical assumptions andassumption †

(concerning non-splitting of a cocycle derived from h), we have

Ge006= eG000.

(50)

Connected components: meta-example

Theorem (Gismatullin, Krupi ´nski 2012) 0 → A → eG→ G → 0π A, G: definable groups (A abelian),

G = A × G:e definable group in terms of 2-cocyle h : G2→ A.

Under some technical assumptions andassumption †

(concerning non-splitting of a cocycle derived from h), we have

Ge006= eG000.

(51)

Main theorem for definable group extensions

Theorem

Suppose we have:

H E ee G: Fσ normal subgroup;

H ∩ A and π[ ee H]: type-definable;

(technical assumptions).

Then eH is type-definable.

Proof.

Using the technical theorem and a certain topology (weaker than Vietoris) on subsets of A/(A ∩ eH).

(52)

Main theorem for definable group extensions

Theorem

Suppose we have:

H E ee G: Fσ normal subgroup;

H ∩ A and π[ ee H]: type-definable;

(technical assumptions).

Then eH is type-definable.

Proof.

Using the technical theorem and a certain topology (weaker than Vietoris) on subsets of A/(A ∩ eH).

(53)

Main theorem for definable group extensions

Theorem

Suppose we have:

H E ee G: Fσ normal subgroup;

H ∩ A and π[ ee H]: type-definable;

(technical assumptions).

Then eH is type-definable.

Proof.

Using the technical theorem and a certain topology (weaker than Vietoris) on subsets of A/(A ∩ eH).

(54)

Main theorem for definable group extensions

Theorem

Suppose we have:

H E ee G: Fσ normal subgroup;

H ∩ A and π[ ee H]: type-definable;

(technical assumptions).

Then eH is type-definable.

Proof.

Using the technical theorem and a certain topology (weaker than Vietoris) on subsets of A/(A ∩ eH).

(55)

Main theorem for definable group extensions

Theorem

Suppose we have:

H E ee G: Fσ normal subgroup;

H ∩ A and π[ ee H]: type-definable;

(technical assumptions).

Then eH is type-definable.

Proof.

Using the technical theorem and a certain topology (weaker than Vietoris) on subsets of A/(A ∩ eH).

(56)

Corollary

Question (Gismatullin & Krupi ´nski 2012)

In the meta-example, if G00=G000, does eG0006= eG00 imply assumption †?

Corollary (with some natural assumptions) Yes!

Moreover, if G00 =G000, then

Ge00/ eG000∼= K /D

where K is a compact group and D is finitely generated dense.

(57)

Corollary

Question (Gismatullin & Krupi ´nski 2012)

In the meta-example, if G00=G000, does eG0006= eG00 imply assumption †?

Corollary (with some natural assumptions) Yes!

Moreover, if G00 =G000, then

Ge00/ eG000∼= K /D

where K is a compact group and D is finitely generated dense.

(58)

Infinite diameter is independent of n.f. (usually)

Example

T = Th(R, +, ·, 0, 1), E – total relation, Φn(x , y ) =W

n

V

m≥n(x = m ↔ y = m) is a normal form for E ,

E has only one class, which has infinite diameter w.r.t.

W

nΦn;

the only class clearly has diameter 1 with respect to trivial normal form Φ0n(x , y ) = >

E does not refine ≡.

(59)

Example

G = h(1, 2)(3, 5)(4, 6), (1, 3, 6)(2, 4, 5)i

= {(), (1, 2)(3, 5)(4, 6), (1, 3, 6)(2, 4, 5),

(1, 4)(2, 3)(5, 6), (1, 5)(2, 6)(3, 4), (1, 6, 3)(2, 5, 4)}

1 ∼ 2, 3 ∼ 4, 5 ∼ 6 (and no other nontrivial relations) M: (finite) structure such that G is the automorphism group and ∼ is definable.

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