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Standard universal dendrites as small Polish structures

(2)

The concept of small Polish structures has been introduced and studied in K. Krupi´ nski, Some model theory of Polish structures, TAMS

Goals:

▸ Provide a setting which allows simultaneous application of ideas and techniques from model theory and descriptive set theory.

In particular:

▸ prove counterparts of some results from stability theory;

▸ find, in this wider context, counterexamples to open problems;

▸ provide a (yet another) tool to measure complexity of dinamycal

systems.

(3)

The concept of small Polish structures has been introduced and studied in K. Krupi´ nski, Some model theory of Polish structures, TAMS

Goals:

▸ Provide a setting which allows simultaneous application of ideas and techniques from model theory and descriptive set theory.

In particular:

▸ prove counterparts of some results from stability theory;

▸ find, in this wider context, counterexamples to open problems;

▸ provide a (yet another) tool to measure complexity of dinamycal

systems.

(4)

The concept of small Polish structures has been introduced and studied in K. Krupi´ nski, Some model theory of Polish structures, TAMS

Goals:

▸ Provide a setting which allows simultaneous application of ideas and techniques from model theory and descriptive set theory.

In particular:

▸ prove counterparts of some results from stability theory;

▸ find, in this wider context, counterexamples to open problems;

▸ provide a (yet another) tool to measure complexity of dinamycal

systems.

(5)

The concept of small Polish structures has been introduced and studied in K. Krupi´ nski, Some model theory of Polish structures, TAMS

Goals:

▸ Provide a setting which allows simultaneous application of ideas and techniques from model theory and descriptive set theory.

In particular:

▸ prove counterparts of some results from stability theory;

▸ find, in this wider context, counterexamples to open problems;

▸ provide a (yet another) tool to measure complexity of dinamycal

systems.

(6)

The concept of small Polish structures has been introduced and studied in K. Krupi´ nski, Some model theory of Polish structures, TAMS

Goals:

▸ Provide a setting which allows simultaneous application of ideas and techniques from model theory and descriptive set theory.

In particular:

▸ prove counterparts of some results from stability theory;

▸ find, in this wider context, counterexamples to open problems;

▸ provide a (yet another) tool to measure complexity of dinamycal

systems.

(7)

Polish structures

A Polish structure is a pair (X , G) where:

▸ G is a Polish group acting faithfully on a set X i.e ∀g, g ∈ G (g ≠ g ⇒ ∃a ∈ X ga ≠ g a )

▸ the stabilisers of all singletons are closed

This generalises the notion of a profinite structure.

Notation: For A ⊆ X , G A will denote the pointwise stabiliser of A.

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Polish structures

A Polish structure is a pair (X , G) where:

▸ G is a Polish group acting faithfully on a set X i.e ∀g, g ∈ G (g ≠ g ⇒ ∃a ∈ X ga ≠ g a )

▸ the stabilisers of all singletons are closed This generalises the notion of a profinite structure.

Notation: For A ⊆ X , G A will denote the pointwise stabiliser of A.

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Polish structures

A Polish structure is a pair (X , G) where:

▸ G is a Polish group acting faithfully on a set X i.e ∀g, g ∈ G (g ≠ g ⇒ ∃a ∈ X ga ≠ g a )

▸ the stabilisers of all singletons are closed This generalises the notion of a profinite structure.

Notation: For A ⊆ X , G A will denote the pointwise stabiliser of A.

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Independence

A notion of independence in Polish structures is introduce.

Let ⃗a ∈ X and A ⊆ B ⊆ X finite.

The idea is to say that ⃗a is independent from B over A if, once A has been fixed, asking to fix B does not add too much constraint on ⃗a, i.e.

G B ⃗a is big in G A ⃗a.

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Some topological notions of bigness: Open, non-meagre,...

However:

● X does not necessarily have a topology.

● Even if X has a nice topology, some orbits G A ⃗a might behave badly, like being meagre in themselves.

Thus the relations of independence are defined via a pull back to the

group G .

(12)

Some topological notions of bigness: Open, non-meagre,...

However:

● X does not necessarily have a topology.

● Even if X has a nice topology, some orbits G A ⃗a might behave badly, like being meagre in themselves.

Thus the relations of independence are defined via a pull back to the

group G .

(13)

Some topological notions of bigness: Open, non-meagre,...

However:

● X does not necessarily have a topology.

● Even if X has a nice topology, some orbits G A ⃗a might behave badly, like being meagre in themselves.

Thus the relations of independence are defined via a pull back to the

group G .

(14)

Some topological notions of bigness: Open, non-meagre,...

However:

● X does not necessarily have a topology.

● Even if X has a nice topology, some orbits G A ⃗a might behave badly, like being meagre in themselves.

Thus the relations of independence are defined via a pull back to the

group G .

(15)

Let π A ∶ G A → G A ⃗a and check whether g ↦ g⃗a

π −1 A (G B ⃗a) is big in π −1 A (G A ⃗a) = G A .

Definitions.

Let ⃗a ∈ X and A, B ⊆ fin X (most often A ⊆ B).

⃗a ⌣∣ o A B: ⃗a is o-independent from B over A if π A −1 (G A∪B ⃗a) is open in G A

(written π −1 A (G A∪B ⃗a) ⊆ o G A ).

⃗a ⌣∣ nm A B: ⃗a is nm-independent from B over A if π −1 A (G A∪B ⃗a) is non-meagre in G A (written π A −1 (G A∪B ⃗a) ⊆ nm G A ).

Remark. If X is separable metrisable, the action G × X → X is continuous and G A ⃗a is not meagre in itself, then

⃗a A B ⇔ G A∪B ⃗a ⊆ G A ⃗a

(for ∗ = nm it is enough X being Hausdorff)

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Let π A ∶ G A → G A ⃗a and check whether g ↦ g⃗a

π −1 A (G B ⃗a) is big in π −1 A (G A ⃗a) = G A . Definitions.

Let ⃗a ∈ X and A, B ⊆ fin X (most often A ⊆ B).

⃗a ⌣∣ o A B: ⃗a is o-independent from B over A if π A −1 (G A∪B ⃗a) is open in G A

(written π −1 A (G A∪B ⃗a) ⊆ o G A ).

⃗a ⌣∣ nm A B: ⃗a is nm-independent from B over A if π −1 A (G A∪B ⃗a) is non-meagre in G A (written π A −1 (G A∪B ⃗a) ⊆ nm G A ).

Remark. If X is separable metrisable, the action G × X → X is continuous and G A ⃗a is not meagre in itself, then

⃗a A B ⇔ G A∪B ⃗a ⊆ G A ⃗a

(for ∗ = nm it is enough X being Hausdorff)

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Let π A ∶ G A → G A ⃗a and check whether g ↦ g⃗a

π −1 A (G B ⃗a) is big in π −1 A (G A ⃗a) = G A . Definitions.

Let ⃗a ∈ X and A, B ⊆ fin X (most often A ⊆ B).

⃗a ⌣∣ o A B: ⃗a is o-independent from B over A if π A −1 (G A∪B ⃗a) is open in G A

(written π −1 A (G A∪B ⃗a) ⊆ o G A ).

⃗a ⌣∣ nm A B: ⃗a is nm-independent from B over A if π −1 A (G A∪B ⃗a) is non-meagre in G A (written π A −1 (G A∪B ⃗a) ⊆ nm G A ).

Remark. If X is separable metrisable, the action G × X → X is continuous and G A ⃗a is not meagre in itself, then

⃗a A B ⇔ G A∪B ⃗a ⊆ G A ⃗a

(for ∗ = nm it is enough X being Hausdorff)

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Example: A = ∅.

⃗a ⌣∣ B iff {g ∈ G ∣ ∃h ∈ G B g ⃗a = h⃗a} ⊆ G

The opposite situation: small orbits. Let A ⊆ fin X .

▸ dcl (A) = {a ∈ X ∣ G A a = {a}}: definable closure of A

▸ acl (A) = {a ∈ X ∣ G A a is finite }: strong algebraic closure of A

▸ Acl (A) = {a ∈ X ∣ G A a is at most countable }: algebraic closure of A For any A ⊆ X , define

dcl (A) = ⋃

A

0

fin

X

dcl (A 0 ),

etc.

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Example: A = ∅.

⃗a ⌣∣ B iff {g ∈ G ∣ ∃h ∈ G B g ⃗a = h⃗a} ⊆ G The opposite situation: small orbits. Let A ⊆ fin X .

▸ dcl (A) = {a ∈ X ∣ G A a = {a}}: definable closure of A

▸ acl (A) = {a ∈ X ∣ G A a is finite }: strong algebraic closure of A

▸ Acl (A) = {a ∈ X ∣ G A a is at most countable }: algebraic closure of A For any A ⊆ X , define

dcl (A) = ⋃

A

0

fin

X

dcl (A 0 ),

etc.

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Basic properties of independence

To develop a counterpart of basic geometric stability theory, five properties of the independence relation are needed

▸ Invariance: ⃗a ⌣∣ A B ⇔ g⃗a ⌣∣ gA gB

▸ Simmetry: ⃗a ⌣∣ A ⃗b ⇔ ⃗b ⌣∣ A ⃗a

▸ Transitivity: ⃗a ⌣∣ A B ∧ ⃗a ⌣∣ B C ⇔ ⃗a ⌣∣ A C

▸ a ∈ Acl(A) ⇔ ∀B ⃗a ⌣∣ A B

▸ Existence of independent extensions

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Small Polish structures

A Polish structure (X , G) is small if

∀n, G × X n → X n has at most countably many orbits

(iff ∀a 1 , . . . , a n ∈ X , G a

1

,...,a

n

× X → X has at most countably many orbits)

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Small Polish structures

A Polish structure (X , G) is small if

∀n, G × X n → X n has at most countably many orbits

(iff ∀a 1 , . . . , a n ∈ X , G a

1

,...,a

n

× X → X has at most countably many orbits)

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Existence of independent extensions

Theorem. Let (X , G) be a small Polish structure. Then

∀⃗a, ∀A ⊆ B ⊆ fin X ,

∃⃗b ∈ G A ⃗a such that

⃗b ⌣∣ nm A B

Remark. The same is not true for o-independent extensions.

(24)

Existence of independent extensions

Theorem. Let (X , G) be a small Polish structure. Then

∀⃗a, ∀A ⊆ B ⊆ fin X , ∃⃗b ∈ G A ⃗a

such that

⃗b ⌣∣ nm A B

Remark. The same is not true for o-independent extensions.

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Existence of independent extensions

Theorem. Let (X , G) be a small Polish structure. Then

∀⃗a, ∀A ⊆ B ⊆ fin X , ∃⃗b ∈ G A ⃗a such that

⃗b ⌣∣ nm A B

Remark. The same is not true for o-independent extensions.

(26)

Existence of independent extensions

Theorem. Let (X , G) be a small Polish structure. Then

∀⃗a, ∀A ⊆ B ⊆ fin X , ∃⃗b ∈ G A ⃗a such that

⃗b ⌣∣ nm A B

Remark. The same is not true for o-independent extensions.

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Adaptation of some concepts from stability theory

▸ X eq = ⋃{X n /E ∣E invariant eq. rel. on X n , s.t Stab ([a] E ) ≤ c G }, the imaginary extension of X

▸ Sets X n /E are the sorts of X eq

▸ D ⊆ X n /E, for X n /E a sort, is definable on A ⊆ fin X eq if G A D = D and Stab (D) ≤ c G

▸ d ∈ X eq is a name for D if ∀g ∈ G (gD = D ⇔ gd = d)

Proposition. Every definable set in X eq has a name in X eq .

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Adaptation of some concepts from stability theory

▸ X eq = ⋃{X n /E ∣E invariant eq. rel. on X n , s.t Stab ([a] E ) ≤ c G }, the imaginary extension of X

▸ Sets X n /E are the sorts of X eq

▸ D ⊆ X n /E, for X n /E a sort, is definable on A ⊆ fin X eq if G A D = D and Stab (D) ≤ c G

▸ d ∈ X eq is a name for D if ∀g ∈ G (gD = D ⇔ gd = d)

Proposition. Every definable set in X eq has a name in X eq .

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Adaptation of some concepts from stability theory

▸ X eq = ⋃{X n /E ∣E invariant eq. rel. on X n , s.t Stab ([a] E ) ≤ c G }, the imaginary extension of X

▸ Sets X n /E are the sorts of X eq

▸ D ⊆ X n /E, for X n /E a sort, is definable on A ⊆ fin X eq if G A D = D and Stab (D) ≤ c G

▸ d ∈ X eq is a name for D if ∀g ∈ G (gD = D ⇔ gd = d)

Proposition. Every definable set in X eq has a name in X eq .

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Adaptation of some concepts from stability theory

▸ X eq = ⋃{X n /E ∣E invariant eq. rel. on X n , s.t Stab ([a] E ) ≤ c G }, the imaginary extension of X

▸ Sets X n /E are the sorts of X eq

▸ D ⊆ X n /E, for X n /E a sort, is definable on A ⊆ fin X eq if G A D = D and Stab (D) ≤ c G

▸ d ∈ X eq is a name for D if ∀g ∈ G (gD = D ⇔ gd = d)

Proposition. Every definable set in X eq has a name in X eq .

(31)

Adaptation of some concepts from stability theory

▸ X eq = ⋃{X n /E ∣E invariant eq. rel. on X n , s.t Stab ([a] E ) ≤ c G }, the imaginary extension of X

▸ Sets X n /E are the sorts of X eq

▸ D ⊆ X n /E, for X n /E a sort, is definable on A ⊆ fin X eq if G A D = D and Stab (D) ≤ c G

▸ d ∈ X eq is a name for D if ∀g ∈ G (gD = D ⇔ gd = d)

Proposition. Every definable set in X eq has a name in X eq .

(32)

Adaptation of some concepts from stability theory

▸ X eq = ⋃{X n /E ∣E invariant eq. rel. on X n , s.t Stab ([a] E ) ≤ c G }, the imaginary extension of X

▸ Sets X n /E are the sorts of X eq

▸ D ⊆ X n /E, for X n /E a sort, is definable on A ⊆ fin X eq if G A D = D and Stab (D) ≤ c G

▸ d ∈ X eq is a name for D if ∀g ∈ G (gD = D ⇔ gd = d)

Proposition. Every definable set in X eq has a name in X eq .

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Ranks

Assume (X , G) is a small Polish structure (but in most situations it is enough to ask for the existence of nm-independent extensions)

Definition. N M is the function from the collection of orbits over finite sets (in X or X eq ) to Ord ∪ {∞},

N M ∶ (a, A) ↦ N M(a, A) ∈ Ord ∪ {∞} satisfying

N M(a, A) ≥ α + 1 ⇔ ∃B ⊇ fin A (N M(a, B) ≥ α ∧ ¬a ⌣∣ nm A B )

Example. N M(a, A) = 0 ⇔ a ∈ Acl eq (A).

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Ranks

Assume (X , G) is a small Polish structure (but in most situations it is enough to ask for the existence of nm-independent extensions)

Definition. N M is the function from the collection of orbits over finite sets (in X or X eq ) to Ord ∪ {∞},

N M ∶ (a, A) ↦ N M(a, A) ∈ Ord ∪ {∞}

satisfying

N M(a, A) ≥ α + 1 ⇔ ∃B ⊇ fin A (N M(a, B) ≥ α ∧ ¬a ⌣∣ nm A B )

Example. N M(a, A) = 0 ⇔ a ∈ Acl eq (A).

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Ranks

Assume (X , G) is a small Polish structure (but in most situations it is enough to ask for the existence of nm-independent extensions)

Definition. N M is the function from the collection of orbits over finite sets (in X or X eq ) to Ord ∪ {∞},

N M ∶ (a, A) ↦ N M(a, A) ∈ Ord ∪ {∞}

satisfying

N M(a, A) ≥ α + 1 ⇔ ∃B ⊇ fin A (N M(a, B) ≥ α ∧ ¬a ⌣∣ nm A B )

Example. N M(a, A) = 0 ⇔ a ∈ Acl eq (A).

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Definition. (X , G) is nm-stable if every 1-orbit has ordinal rank, i.e.

there is no infinite sequence A 0 ⊆ A 1 ⊆ . . . ⊆ fin X and a ∈ X such that a is nm-dependent from A i +1 over A i .

Definition. If D is definable over A in X eq , the N M-rank of D is

N M(D) = sup{N M(d, A) ∣ d ∈ D}

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Definition. (X , G) is nm-stable if every 1-orbit has ordinal rank, i.e.

there is no infinite sequence A 0 ⊆ A 1 ⊆ . . . ⊆ fin X and a ∈ X such that a is nm-dependent from A i +1 over A i .

Definition. If D is definable over A in X eq , the N M-rank of D is

N M(D) = sup{N M(d, A) ∣ d ∈ D}

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Examples (Krupi´ nski)

▸ (S n , Homeo (S n )) has rank 1

▸ ((S 1 ) n , Homeo ((S 1 ) n )) has rank 1

▸ ([0, 1] N , Homeo ([0, 1] N )) has rank 1

▸ if (X , G) has rank 1, then (X n , G ) has rank n

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Continua

Definitions.

▸ A continuum is a compact connected metric space; it is non-degenerate if it has more than one point

▸ A non-degenerate continuum X is decomposable if X = Y ∪ Z, for Y , Z some proper subcontinua of X . Otherwise it is indecomposable

▸ A non-degenerate continuum is hereditarily (in)decomposable if all

its subcontinua are (in)decomposable

(40)

Continua

Definitions.

▸ A continuum is a compact connected metric space; it is non-degenerate if it has more than one point

▸ A non-degenerate continuum X is decomposable if X = Y ∪ Z, for Y , Z some proper subcontinua of X . Otherwise it is indecomposable

▸ A non-degenerate continuum is hereditarily (in)decomposable if all

its subcontinua are (in)decomposable

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Continua

Definitions.

▸ A continuum is a compact connected metric space; it is non-degenerate if it has more than one point

▸ A non-degenerate continuum X is decomposable if X = Y ∪ Z, for Y , Z some proper subcontinua of X . Otherwise it is indecomposable

▸ A non-degenerate continuum is hereditarily (in)decomposable if all

its subcontinua are (in)decomposable

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The pseudo-arc

Definition. The pseudo-arc is the unique continuum that is hereditarily indecomposable and arc-like:

∀ε, ∃f ∶ P ↠ [0, 1] continuous , ∀y, diam(f −1 (y)) < ε

A construction of the pseudoarc:

Fix distinct point p, q ∈ R 2 .

Step 0 Draw a simple chain U 0 = {U 00 , . . . , U 0r

0

} from p to q of

connected open sets of diameter less than 1. Being a simple chain from p to q means:

▸ U i ∩ U j ⇔ ∣i − j∣ ≤ 1

▸ p ∈ U 0i ⇔ i = 0

▸ q ∈ U 0i ⇔ i = r 0

(43)

The pseudo-arc

Definition. The pseudo-arc is the unique continuum that is hereditarily indecomposable and arc-like:

∀ε, ∃f ∶ P ↠ [0, 1] continuous , ∀y, diam(f −1 (y)) < ε

A construction of the pseudoarc:

Fix distinct point p, q ∈ R 2 .

Step 0 Draw a simple chain U 0 = {U 00 , . . . , U 0r

0

} from p to q of

connected open sets of diameter less than 1. Being a simple chain from p to q means:

▸ U i ∩ U j ⇔ ∣i − j∣ ≤ 1

▸ p ∈ U 0i ⇔ i = 0

▸ q ∈ U 0i ⇔ i = r 0

(44)

The pseudo-arc

Definition. The pseudo-arc is the unique continuum that is hereditarily indecomposable and arc-like:

∀ε, ∃f ∶ P ↠ [0, 1] continuous , ∀y, diam(f −1 (y)) < ε

A construction of the pseudoarc:

Fix distinct point p, q ∈ R 2 .

Step 0 Draw a simple chain U 0 = {U 00 , . . . , U 0r

0

} from p to q of

connected open sets of diameter less than 1. Being a simple chain from p to q means:

▸ U i ∩ U j ⇔ ∣i − j∣ ≤ 1

▸ p ∈ U 0i ⇔ i = 0

▸ q ∈ U 0i ⇔ i = r 0

(45)

Step k+1 Draw a simple chain U k+1 = {U k+1,0 , . . . , U k+1,r

k+1

} from p to q of connected open sets of diameter less than k+2 1 such that

▸ the closure of each link of U k+1 is contained in some link of U k

▸ U k+1 is crooked in U k

This last condition means that for all i , j , m, n, if

m + 2 < n, U k+1,i ∩ U km ≠ ∅, U k+1,j ∩ U kn ≠ ∅ then there are s, t with i < s < t < j or i > t > l > j such that

U k+1,s ⊆ U k,n−1 and U k+1,t ⊆ U k,m+1

Final step P = ⋂ k∈N ⋃ U k is the pseudoarc.

(46)

Step k+1 Draw a simple chain U k+1 = {U k+1,0 , . . . , U k+1,r

k+1

} from p to q of connected open sets of diameter less than k+2 1 such that

▸ the closure of each link of U k+1 is contained in some link of U k

▸ U k+1 is crooked in U k

This last condition means that for all i , j , m, n, if

m + 2 < n, U k+1,i ∩ U km ≠ ∅, U k+1,j ∩ U kn ≠ ∅ then there are s, t with i < s < t < j or i > t > l > j such that

U k+1,s ⊆ U k,n−1 and U k+1,t ⊆ U k,m+1

Final step P = ⋂ k∈N ⋃ U k is the pseudoarc.

(47)

Step k+1 Draw a simple chain U k+1 = {U k+1,0 , . . . , U k+1,r

k+1

} from p to q of connected open sets of diameter less than k+2 1 such that

▸ the closure of each link of U k+1 is contained in some link of U k

▸ U k+1 is crooked in U k

This last condition means that for all i , j , m, n, if

m + 2 < n, U k+1,i ∩ U km ≠ ∅, U k+1,j ∩ U kn ≠ ∅

then there are s, t with i < s < t < j or i > t > l > j such that U k+1,s ⊆ U k,n−1 and U k+1,t ⊆ U k,m+1

Final step P = ⋂ k∈N ⋃ U k is the pseudoarc.

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Step k+1 Draw a simple chain U k+1 = {U k+1,0 , . . . , U k+1,r

k+1

} from p to q of connected open sets of diameter less than k+2 1 such that

▸ the closure of each link of U k+1 is contained in some link of U k

▸ U k+1 is crooked in U k

This last condition means that for all i , j , m, n, if

m + 2 < n, U k+1,i ∩ U km ≠ ∅, U k+1,j ∩ U kn ≠ ∅ then there are s, t with i < s < t < j or i > t > l > j such that

U k+1,s ⊆ U k,n−1 and U k+1,t ⊆ U k,m+1

Final step P = ⋂ k∈N ⋃ U k is the pseudoarc.

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Step k+1 Draw a simple chain U k+1 = {U k+1,0 , . . . , U k+1,r

k+1

} from p to q of connected open sets of diameter less than k+2 1 such that

▸ the closure of each link of U k+1 is contained in some link of U k

▸ U k+1 is crooked in U k

This last condition means that for all i , j , m, n, if

m + 2 < n, U k+1,i ∩ U km ≠ ∅, U k+1,j ∩ U kn ≠ ∅ then there are s, t with i < s < t < j or i > t > l > j such that

U k+1,s ⊆ U k,n−1 and U k+1,t ⊆ U k,m+1

Final step P = ⋂ k∈N ⋃ U k is the pseudoarc.

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The pseudo-arc is a quite complicated continuum. Nevertheless it is the generic continuum: the class of pseudo-arcs is dense G δ in the space of all continua.

Theorem. (Krupi´ nski) Let P be the pseudo-arc. Then (P, Homeo(P)) is a small, not nm-stable, Polish structure.

In particular, the N M-rank of P is ∞.

Moreover P is an example of a small Polish structure not admitting

o-independent extensions.

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The pseudo-arc is a quite complicated continuum. Nevertheless it is the generic continuum: the class of pseudo-arcs is dense G δ in the space of all continua.

Theorem. (Krupi´ nski) Let P be the pseudo-arc. Then (P, Homeo(P)) is a small, not nm-stable, Polish structure.

In particular, the N M-rank of P is ∞.

Moreover P is an example of a small Polish structure not admitting

o-independent extensions.

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The pseudo-arc is a quite complicated continuum. Nevertheless it is the generic continuum: the class of pseudo-arcs is dense G δ in the space of all continua.

Theorem. (Krupi´ nski) Let P be the pseudo-arc. Then (P, Homeo(P)) is a small, not nm-stable, Polish structure.

In particular, the N M-rank of P is ∞.

Moreover P is an example of a small Polish structure not admitting

o-independent extensions.

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Dendrites

Among simplest continua are dendrites.

A dendrite is a locally connected continuum that does not contain simple closed curves.

Definition. Given a point x in a continuum X , its order ord (x, X ) is the smallest cardinal β such that x has a basis of open neighbourhoods whose boundaries have cardinality ≤ β.

All points of a dendrite have order ≤ ℵ 0 . Points of order 1 are called end

points; points of order ≥ 3 are branching points.

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Dendrites

Among simplest continua are dendrites.

A dendrite is a locally connected continuum that does not contain simple closed curves.

Definition. Given a point x in a continuum X , its order ord (x, X ) is the smallest cardinal β such that x has a basis of open neighbourhoods whose boundaries have cardinality ≤ β.

All points of a dendrite have order ≤ ℵ 0 . Points of order 1 are called end

points; points of order ≥ 3 are branching points.

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Dendrites

Among simplest continua are dendrites.

A dendrite is a locally connected continuum that does not contain simple closed curves.

Definition. Given a point x in a continuum X , its order ord (x, X ) is the smallest cardinal β such that x has a basis of open neighbourhoods whose boundaries have cardinality ≤ β.

All points of a dendrite have order ≤ ℵ 0 . Points of order 1 are called end

points; points of order ≥ 3 are branching points.

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The following property might help to visualise a dendrite:

If X is a non-degenerate dendrite, then X = ⋃

i ∈N

A i ∪ E(X ) where:

▸ each A i is an arc, with end points p i , q i

▸ A i +1 ∩ ⋃ i j =0 A j = {p i +1 }

▸ diam (A i ) → 0

▸ E (X ) is the set of end points of X

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The goal is to study Polish structures of the form (D, Homeo(D)) where D is a dendrite.

Remark. Not all dendrites are small Polish structures. Let D ⊆ R 2 be obtained by starting with [0, 1] × {0} as follows:

▸ enumerate {q n } n∈N = (]0, 1[∩Q) × {0}

▸ at step n add n arcs of diameter ≤ 2 1

n

intersecting each other and the already achieved construction only in q n

Then all point of ]0, 1[×{0} are in distinct orbits.

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The goal is to study Polish structures of the form (D, Homeo(D)) where D is a dendrite.

Remark. Not all dendrites are small Polish structures. Let D ⊆ R 2 be obtained by starting with [0, 1] × {0} as follows:

▸ enumerate {q n } n∈N = (]0, 1[∩Q) × {0}

▸ at step n add n arcs of diameter ≤ 2 1

n

intersecting each other and the already achieved construction only in q n

Then all point of ]0, 1[×{0} are in distinct orbits.

(59)

The goal is to study Polish structures of the form (D, Homeo(D)) where D is a dendrite.

Remark. Not all dendrites are small Polish structures. Let D ⊆ R 2 be obtained by starting with [0, 1] × {0} as follows:

▸ enumerate {q n } n∈N = (]0, 1[∩Q) × {0}

▸ at step n add n arcs of diameter ≤ 2 1

n

intersecting each other and the already achieved construction only in q n

Then all point of ]0, 1[×{0} are in distinct orbits.

(60)

The goal is to study Polish structures of the form (D, Homeo(D)) where D is a dendrite.

Remark. Not all dendrites are small Polish structures. Let D ⊆ R 2 be obtained by starting with [0, 1] × {0} as follows:

▸ enumerate {q n } n∈N = (]0, 1[∩Q) × {0}

▸ at step n add n arcs of diameter ≤ 2 1

n

intersecting each other and the already achieved construction only in q n

Then all point of ]0, 1[×{0} are in distinct orbits.

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Wa˙zewski’s universal dendrites

Let ∅ ≠ J ⊆ {3, 4 . . . , ω}.

There is a unique dendrite D J such that

▸ each branching point of D J has order in J

▸ each subarc of D J contains points of any order in J

Universality property

D J is universal for the class of dendrites whose branching points have

order in J: any such dendrite embeds in D J .

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Wa˙zewski’s universal dendrites

Let ∅ ≠ J ⊆ {3, 4 . . . , ω}.

There is a unique dendrite D J such that

▸ each branching point of D J has order in J

▸ each subarc of D J contains points of any order in J Universality property

D J is universal for the class of dendrites whose branching points have

order in J: any such dendrite embeds in D J .

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Theorem. Each (D J , Homeo (D J )) is a small Polish structure of N M-rank 1

Conjectures.

▸ Each dendrite admits nm-independent extensions

▸ If D is a dendrite and (D, Homeo(D)) is small, then N M(D) = 1

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Theorem. Each (D J , Homeo (D J )) is a small Polish structure of N M-rank 1

Conjectures.

▸ Each dendrite admits nm-independent extensions

▸ If D is a dendrite and (D, Homeo(D)) is small, then N M(D) = 1

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Some questions.

▸ Characterise dendrites D such that (D, Homeo(D)) is small.

▸ Find examples of continua C with 1 < N M(C) < ∞.

▸ The N M-gap conjecture.

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Some questions.

▸ Characterise dendrites D such that (D, Homeo(D)) is small.

▸ Find examples of continua C with 1 < N M(C) < ∞.

▸ The N M-gap conjecture.

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Some questions.

▸ Characterise dendrites D such that (D, Homeo(D)) is small.

▸ Find examples of continua C with 1 < N M(C) < ∞.

▸ The N M-gap conjecture.

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An example of a small Polish structure (X , G) with N M(X ) = ω can be obtained as a disjoint sum of small Polish structures of increasing natural rank.

E.g., take (Y , G) of rank 1 an let X = ⋃ n≥1 X n .

However, in this example the is no single orbit over finite sets with rank

≥ ω (and ≠ ∞).

The N M-gap conjecture. Let (X , G) be a small Polish structure. Then, for any orbit o of a finite set A ⊆ X , one has

N M(o) ∈ ω ∪ {∞}.

This conjecture is open in the class of small profinite structures; it has

been proved for small m-stable profinite groups. In this wider context it

might be easier to find a counterexample.

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An example of a small Polish structure (X , G) with N M(X ) = ω can be obtained as a disjoint sum of small Polish structures of increasing natural rank.

E.g., take (Y , G) of rank 1 an let X = ⋃ n≥1 X n .

However, in this example the is no single orbit over finite sets with rank

≥ ω (and ≠ ∞).

The N M-gap conjecture. Let (X , G) be a small Polish structure. Then, for any orbit o of a finite set A ⊆ X , one has

N M(o) ∈ ω ∪ {∞}.

This conjecture is open in the class of small profinite structures; it has

been proved for small m-stable profinite groups. In this wider context it

might be easier to find a counterexample.

(70)

An example of a small Polish structure (X , G) with N M(X ) = ω can be obtained as a disjoint sum of small Polish structures of increasing natural rank.

E.g., take (Y , G) of rank 1 an let X = ⋃ n≥1 X n .

However, in this example the is no single orbit over finite sets with rank

≥ ω (and ≠ ∞).

The N M-gap conjecture. Let (X , G) be a small Polish structure.

Then, for any orbit o of a finite set A ⊆ X , one has N M(o) ∈ ω ∪ {∞}.

This conjecture is open in the class of small profinite structures; it has

been proved for small m-stable profinite groups. In this wider context it

might be easier to find a counterexample.

(71)

An example of a small Polish structure (X , G) with N M(X ) = ω can be obtained as a disjoint sum of small Polish structures of increasing natural rank.

E.g., take (Y , G) of rank 1 an let X = ⋃ n≥1 X n .

However, in this example the is no single orbit over finite sets with rank

≥ ω (and ≠ ∞).

The N M-gap conjecture. Let (X , G) be a small Polish structure.

Then, for any orbit o of a finite set A ⊆ X , one has N M(o) ∈ ω ∪ {∞}.

This conjecture is open in the class of small profinite structures; it has

been proved for small m-stable profinite groups. In this wider context it

might be easier to find a counterexample.

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