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Combinatorial properties of singular cardinals Dima Sinapova University of Illinois at Chicago August 2013 Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals Overview Singular cardinals Dima


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Combinatorial properties of singular cardinals

Dima Sinapova University of Illinois at Chicago August 2013

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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Overview

◮ Singular cardinals

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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Overview

◮ Singular cardinals ◮ Consistency results

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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Overview

◮ Singular cardinals ◮ Consistency results ◮ Large cardinals

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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Overview

◮ Singular cardinals ◮ Consistency results ◮ Large cardinals ◮ Prikry forcing constructions

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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Overview

◮ Singular cardinals ◮ Consistency results ◮ Large cardinals ◮ Prikry forcing constructions ◮ Conbinatorial principles

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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Cardinal arithmetic

The cardinals are indexed ℵα : α ∈ Ord.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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Cardinal arithmetic

The cardinals are indexed ℵα : α ∈ Ord.

◮ The smallest infinite cardinal is ω (or ℵ0).

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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Cardinal arithmetic

The cardinals are indexed ℵα : α ∈ Ord.

◮ The smallest infinite cardinal is ω (or ℵ0). ◮ Next is ω1 (or ℵ1); the least uncountable cardinal.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 10

Cardinal arithmetic

The cardinals are indexed ℵα : α ∈ Ord.

◮ The smallest infinite cardinal is ω (or ℵ0). ◮ Next is ω1 (or ℵ1); the least uncountable cardinal. ◮ Each cardinal is also a set. E.g. ℵ1 = {α | α is countable}

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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Cardinal arithmetic

The cardinals are indexed ℵα : α ∈ Ord.

◮ The smallest infinite cardinal is ω (or ℵ0). ◮ Next is ω1 (or ℵ1); the least uncountable cardinal. ◮ Each cardinal is also a set. E.g. ℵ1 = {α | α is countable} ◮ And so we have: 0, 1, ..., ℵ0, ℵ1, ..., ℵn, ..., ℵω, ℵω+1, ...

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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Cardinal arithmetic

The cardinals are indexed ℵα : α ∈ Ord.

◮ The smallest infinite cardinal is ω (or ℵ0). ◮ Next is ω1 (or ℵ1); the least uncountable cardinal. ◮ Each cardinal is also a set. E.g. ℵ1 = {α | α is countable} ◮ And so we have: 0, 1, ..., ℵ0, ℵ1, ..., ℵn, ..., ℵω, ℵω+1, ... ◮ Arithmetic operations on cardinals:

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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Cardinal arithmetic

The cardinals are indexed ℵα : α ∈ Ord.

◮ The smallest infinite cardinal is ω (or ℵ0). ◮ Next is ω1 (or ℵ1); the least uncountable cardinal. ◮ Each cardinal is also a set. E.g. ℵ1 = {α | α is countable} ◮ And so we have: 0, 1, ..., ℵ0, ℵ1, ..., ℵn, ..., ℵω, ℵω+1, ... ◮ Arithmetic operations on cardinals:

◮ κ + λ is size of disjoint union of κ and λ; Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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Cardinal arithmetic

The cardinals are indexed ℵα : α ∈ Ord.

◮ The smallest infinite cardinal is ω (or ℵ0). ◮ Next is ω1 (or ℵ1); the least uncountable cardinal. ◮ Each cardinal is also a set. E.g. ℵ1 = {α | α is countable} ◮ And so we have: 0, 1, ..., ℵ0, ℵ1, ..., ℵn, ..., ℵω, ℵω+1, ... ◮ Arithmetic operations on cardinals:

◮ κ + λ is size of disjoint union of κ and λ; ◮ κ · λ is size of Cartesian product; Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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Cardinal arithmetic

The cardinals are indexed ℵα : α ∈ Ord.

◮ The smallest infinite cardinal is ω (or ℵ0). ◮ Next is ω1 (or ℵ1); the least uncountable cardinal. ◮ Each cardinal is also a set. E.g. ℵ1 = {α | α is countable} ◮ And so we have: 0, 1, ..., ℵ0, ℵ1, ..., ℵn, ..., ℵω, ℵω+1, ... ◮ Arithmetic operations on cardinals:

◮ κ + λ is size of disjoint union of κ and λ; ◮ κ · λ is size of Cartesian product; ◮ κλ is size of the set of functions from λ to κ. Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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Cardinal arithmetic

The cardinals are indexed ℵα : α ∈ Ord.

◮ The smallest infinite cardinal is ω (or ℵ0). ◮ Next is ω1 (or ℵ1); the least uncountable cardinal. ◮ Each cardinal is also a set. E.g. ℵ1 = {α | α is countable} ◮ And so we have: 0, 1, ..., ℵ0, ℵ1, ..., ℵn, ..., ℵω, ℵω+1, ... ◮ Arithmetic operations on cardinals:

◮ κ + λ is size of disjoint union of κ and λ; ◮ κ · λ is size of Cartesian product; ◮ κλ is size of the set of functions from λ to κ.

◮ Fact: if κ, λ are infinite, then κ + λ = κ · λ = max(κ, λ).

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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Cardinal arithmetic

ℵ0, ℵ1, ..., ℵω, ℵω+1, ...

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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Cardinal arithmetic

ℵ0, ℵ1, ..., ℵω, ℵω+1, ... The cofinality of a cardinal κ, cf(κ), is the least τ such that there is an unbounded subset of κ of size τ.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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Cardinal arithmetic

ℵ0, ℵ1, ..., ℵω, ℵω+1, ... The cofinality of a cardinal κ, cf(κ), is the least τ such that there is an unbounded subset of κ of size τ.

◮ For example: cf(ℵn) = ℵn for all n < ω; cf(ℵω) = ω.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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Cardinal arithmetic

ℵ0, ℵ1, ..., ℵω, ℵω+1, ... The cofinality of a cardinal κ, cf(κ), is the least τ such that there is an unbounded subset of κ of size τ.

◮ For example: cf(ℵn) = ℵn for all n < ω; cf(ℵω) = ω. ◮ A cardinal κ is regular if cf(κ) = κ.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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Cardinal arithmetic

ℵ0, ℵ1, ..., ℵω, ℵω+1, ... The cofinality of a cardinal κ, cf(κ), is the least τ such that there is an unbounded subset of κ of size τ.

◮ For example: cf(ℵn) = ℵn for all n < ω; cf(ℵω) = ω. ◮ A cardinal κ is regular if cf(κ) = κ. ◮ A cardinal κ is singular if cf(κ) < κ.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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Cardinal arithmetic

ℵ0, ℵ1, ..., ℵω, ℵω+1, ... The cofinality of a cardinal κ, cf(κ), is the least τ such that there is an unbounded subset of κ of size τ.

◮ For example: cf(ℵn) = ℵn for all n < ω; cf(ℵω) = ω. ◮ A cardinal κ is regular if cf(κ) = κ. ◮ A cardinal κ is singular if cf(κ) < κ. ◮ For example, ℵn is regular for every n, and ℵω is singular.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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Cardinal arithmetic and the exponential operation

Motivating question: analyze behavior of the operation κ → 2κ.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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Cardinal arithmetic and the exponential operation

Motivating question: analyze behavior of the operation κ → 2κ.

◮ (Cantor) 2κ > κ for every cardinal κ.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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Cardinal arithmetic and the exponential operation

Motivating question: analyze behavior of the operation κ → 2κ.

◮ (Cantor) 2κ > κ for every cardinal κ. ◮ (K˝

  • nig) κcf(κ) > κ for every cardinal κ.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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Cardinal arithmetic and the exponential operation

Motivating question: analyze behavior of the operation κ → 2κ.

◮ (Cantor) 2κ > κ for every cardinal κ. ◮ (K˝

  • nig) κcf(κ) > κ for every cardinal κ.

◮ The Continuum Hypothesis (CH): 2ℵ0 = ℵ1.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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Cardinal arithmetic and the exponential operation

Motivating question: analyze behavior of the operation κ → 2κ.

◮ (Cantor) 2κ > κ for every cardinal κ. ◮ (K˝

  • nig) κcf(κ) > κ for every cardinal κ.

◮ The Continuum Hypothesis (CH): 2ℵ0 = ℵ1. ◮ The Generalized Continuum Hypothesis (GCH):

2κ = κ+ for all cardinals κ. (κ+, the successor of κ, is the next bigger cardinal after κ.)

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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Cardinal arithmetic and the exponential operation

Motivating question: analyze behavior of the operation κ → 2κ.

◮ (Cantor) 2κ > κ for every cardinal κ. ◮ (K˝

  • nig) κcf(κ) > κ for every cardinal κ.

◮ The Continuum Hypothesis (CH): 2ℵ0 = ℵ1. ◮ The Generalized Continuum Hypothesis (GCH):

2κ = κ+ for all cardinals κ. (κ+, the successor of κ, is the next bigger cardinal after κ.)

◮ The Singular Cardinal Hypothesis (SCH):

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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Cardinal arithmetic and the exponential operation

Motivating question: analyze behavior of the operation κ → 2κ.

◮ (Cantor) 2κ > κ for every cardinal κ. ◮ (K˝

  • nig) κcf(κ) > κ for every cardinal κ.

◮ The Continuum Hypothesis (CH): 2ℵ0 = ℵ1. ◮ The Generalized Continuum Hypothesis (GCH):

2κ = κ+ for all cardinals κ. (κ+, the successor of κ, is the next bigger cardinal after κ.)

◮ The Singular Cardinal Hypothesis (SCH):

If κ is a singular cardinal such that τ < κ → 2τ < κ i.e. κ is strong limit,

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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Cardinal arithmetic and the exponential operation

Motivating question: analyze behavior of the operation κ → 2κ.

◮ (Cantor) 2κ > κ for every cardinal κ. ◮ (K˝

  • nig) κcf(κ) > κ for every cardinal κ.

◮ The Continuum Hypothesis (CH): 2ℵ0 = ℵ1. ◮ The Generalized Continuum Hypothesis (GCH):

2κ = κ+ for all cardinals κ. (κ+, the successor of κ, is the next bigger cardinal after κ.)

◮ The Singular Cardinal Hypothesis (SCH):

If κ is a singular cardinal such that τ < κ → 2τ < κ i.e. κ is strong limit, then 2κ = κ+.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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Cardinal arithmetic and the exponential operation

Motivating question: analyze behavior of the operation κ → 2κ.

◮ (Cantor) 2κ > κ for every cardinal κ. ◮ (K˝

  • nig) κcf(κ) > κ for every cardinal κ.

◮ The Continuum Hypothesis (CH): 2ℵ0 = ℵ1. ◮ The Generalized Continuum Hypothesis (GCH):

2κ = κ+ for all cardinals κ. (κ+, the successor of κ, is the next bigger cardinal after κ.)

◮ The Singular Cardinal Hypothesis (SCH):

If κ is a singular cardinal such that τ < κ → 2τ < κ i.e. κ is strong limit, then 2κ = κ+.

◮ GCH implies SCH.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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Cardinal arithmetic and the exponential operation

Motivating question: analyze behavior of the operation κ → 2κ.

◮ (Cantor) 2κ > κ for every cardinal κ. ◮ (K˝

  • nig) κcf(κ) > κ for every cardinal κ.

◮ The Continuum Hypothesis (CH): 2ℵ0 = ℵ1. ◮ The Generalized Continuum Hypothesis (GCH):

2κ = κ+ for all cardinals κ. (κ+, the successor of κ, is the next bigger cardinal after κ.)

◮ The Singular Cardinal Hypothesis (SCH):

If κ is a singular cardinal such that τ < κ → 2τ < κ i.e. κ is strong limit, then 2κ = κ+.

◮ GCH implies SCH. ◮ Addressing these questions gave rise to consistency results.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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Cardinal arithmetic and the exponential operation

A consistency result is a theorem that asserts that a given statement is consistent with the usual axioms of set theory i.e the Zermelo-Fraenkel Set Theory with the Axiom of Choice (ZFC).

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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Cardinal arithmetic and the exponential operation

A consistency result is a theorem that asserts that a given statement is consistent with the usual axioms of set theory i.e the Zermelo-Fraenkel Set Theory with the Axiom of Choice (ZFC). Consistency results about regular cardinals.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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Cardinal arithmetic and the exponential operation

A consistency result is a theorem that asserts that a given statement is consistent with the usual axioms of set theory i.e the Zermelo-Fraenkel Set Theory with the Axiom of Choice (ZFC). Consistency results about regular cardinals.

◮ Kurt G¨

  • del: CH is consistent with ZFC. His model was the

Constructible Universe, L, and actually L | = GCH.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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Cardinal arithmetic and the exponential operation

A consistency result is a theorem that asserts that a given statement is consistent with the usual axioms of set theory i.e the Zermelo-Fraenkel Set Theory with the Axiom of Choice (ZFC). Consistency results about regular cardinals.

◮ Kurt G¨

  • del: CH is consistent with ZFC. His model was the

Constructible Universe, L, and actually L | = GCH.

◮ Paul Cohen: The negation of CH is consistent with ZFC. He

used the groundbreaking method of forcing.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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Cardinal arithmetic and the exponential operation

A consistency result is a theorem that asserts that a given statement is consistent with the usual axioms of set theory i.e the Zermelo-Fraenkel Set Theory with the Axiom of Choice (ZFC). Consistency results about regular cardinals.

◮ Kurt G¨

  • del: CH is consistent with ZFC. His model was the

Constructible Universe, L, and actually L | = GCH.

◮ Paul Cohen: The negation of CH is consistent with ZFC. He

used the groundbreaking method of forcing.

◮ Easton: Any reasonable behavior of κ → 2κ for regular κ is

consistent with ZFC.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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Cardinal arithmetic and the exponential operation

A consistency result is a theorem that asserts that a given statement is consistent with the usual axioms of set theory i.e the Zermelo-Fraenkel Set Theory with the Axiom of Choice (ZFC). Consistency results about regular cardinals.

◮ Kurt G¨

  • del: CH is consistent with ZFC. His model was the

Constructible Universe, L, and actually L | = GCH.

◮ Paul Cohen: The negation of CH is consistent with ZFC. He

used the groundbreaking method of forcing.

◮ Easton: Any reasonable behavior of κ → 2κ for regular κ is

consistent with ZFC. The only constraints:

◮ κ < λ implies 2κ ≤ 2λ, ◮ K˝

  • nig’s lemma.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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Cardinal arithmetic and the exponential operation

The operation κ → 2κ for singular κ is much more intricate:

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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Cardinal arithmetic and the exponential operation

The operation κ → 2κ for singular κ is much more intricate:

◮ involves large cardinals, e.g. can violate SCH, but need large

cardinal axioms.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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Cardinal arithmetic and the exponential operation

The operation κ → 2κ for singular κ is much more intricate:

◮ involves large cardinals, e.g. can violate SCH, but need large

cardinal axioms.

◮ deeper constraints from ZFC,

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 42

Cardinal arithmetic and the exponential operation

The operation κ → 2κ for singular κ is much more intricate:

◮ involves large cardinals, e.g. can violate SCH, but need large

cardinal axioms.

◮ deeper constraints from ZFC,

e.g. (Shelah) if 2ℵn < ℵω for every n < ω, then 2ℵω < ℵω4;

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 43

Cardinal arithmetic and the exponential operation

The operation κ → 2κ for singular κ is much more intricate:

◮ involves large cardinals, e.g. can violate SCH, but need large

cardinal axioms.

◮ deeper constraints from ZFC,

e.g. (Shelah) if 2ℵn < ℵω for every n < ω, then 2ℵω < ℵω4; e.g. (Silver) if SCH fails anywhere, it must fail at a cardinal of countable cofinality.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 44

Cardinal arithmetic and the exponential operation

The operation κ → 2κ for singular κ is much more intricate:

◮ involves large cardinals, e.g. can violate SCH, but need large

cardinal axioms.

◮ deeper constraints from ZFC,

e.g. (Shelah) if 2ℵn < ℵω for every n < ω, then 2ℵω < ℵω4; e.g. (Silver) if SCH fails anywhere, it must fail at a cardinal of countable cofinality. The Singular Cardinal Problem: Describe a complete set of rules for the behavior of the exponential function κ → 2κ for singular cardinals κ.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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Using forcing to add new subsets of a cardinal κ

Obtaining consistency results about κ → 2κ is done by forcing to add new subsets of κ.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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Using forcing to add new subsets of a cardinal κ

Obtaining consistency results about κ → 2κ is done by forcing to add new subsets of κ. Forcing: Adjoin a new object to the set-theoretic universe, V .

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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Using forcing to add new subsets of a cardinal κ

Obtaining consistency results about κ → 2κ is done by forcing to add new subsets of κ. Forcing: Adjoin a new object to the set-theoretic universe, V . Start with a ground model V of ZFC and a partially ordered set (P, ≤) ∈ V .

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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Using forcing to add new subsets of a cardinal κ

Obtaining consistency results about κ → 2κ is done by forcing to add new subsets of κ. Forcing: Adjoin a new object to the set-theoretic universe, V . Start with a ground model V of ZFC and a partially ordered set (P, ≤) ∈ V . Pick an object G ⊂ P where:

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 49

Using forcing to add new subsets of a cardinal κ

Obtaining consistency results about κ → 2κ is done by forcing to add new subsets of κ. Forcing: Adjoin a new object to the set-theoretic universe, V . Start with a ground model V of ZFC and a partially ordered set (P, ≤) ∈ V . Pick an object G ⊂ P where:

◮ G is a filter.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 50

Using forcing to add new subsets of a cardinal κ

Obtaining consistency results about κ → 2κ is done by forcing to add new subsets of κ. Forcing: Adjoin a new object to the set-theoretic universe, V . Start with a ground model V of ZFC and a partially ordered set (P, ≤) ∈ V . Pick an object G ⊂ P where:

◮ G is a filter. ◮ G meets every maximal antichain of P.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 51

Using forcing to add new subsets of a cardinal κ

Obtaining consistency results about κ → 2κ is done by forcing to add new subsets of κ. Forcing: Adjoin a new object to the set-theoretic universe, V . Start with a ground model V of ZFC and a partially ordered set (P, ≤) ∈ V . Pick an object G ⊂ P where:

◮ G is a filter. ◮ G meets every maximal antichain of P.

This G is called a generic filter of P, and G / ∈ V .

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

slide-52
SLIDE 52

Using forcing to add new subsets of a cardinal κ

Obtaining consistency results about κ → 2κ is done by forcing to add new subsets of κ. Forcing: Adjoin a new object to the set-theoretic universe, V . Start with a ground model V of ZFC and a partially ordered set (P, ≤) ∈ V . Pick an object G ⊂ P where:

◮ G is a filter. ◮ G meets every maximal antichain of P.

This G is called a generic filter of P, and G / ∈ V . Then obtain the model V [G] of ZFC as follows:

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 53

Using forcing to add new subsets of a cardinal κ

Obtaining consistency results about κ → 2κ is done by forcing to add new subsets of κ. Forcing: Adjoin a new object to the set-theoretic universe, V . Start with a ground model V of ZFC and a partially ordered set (P, ≤) ∈ V . Pick an object G ⊂ P where:

◮ G is a filter. ◮ G meets every maximal antichain of P.

This G is called a generic filter of P, and G / ∈ V . Then obtain the model V [G] of ZFC as follows:

◮ A P-name τ in V is a set of the form

{σ, p | σ is a P-name and p ∈ P}.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 54

Using forcing to add new subsets of a cardinal κ

Obtaining consistency results about κ → 2κ is done by forcing to add new subsets of κ. Forcing: Adjoin a new object to the set-theoretic universe, V . Start with a ground model V of ZFC and a partially ordered set (P, ≤) ∈ V . Pick an object G ⊂ P where:

◮ G is a filter. ◮ G meets every maximal antichain of P.

This G is called a generic filter of P, and G / ∈ V . Then obtain the model V [G] of ZFC as follows:

◮ A P-name τ in V is a set of the form

{σ, p | σ is a P-name and p ∈ P}.

◮ For each P-name τ in V , set τ G = {σG | (∃p ∈ G)σ, p ∈ τ}

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 55

Using forcing to add new subsets of a cardinal κ

Obtaining consistency results about κ → 2κ is done by forcing to add new subsets of κ. Forcing: Adjoin a new object to the set-theoretic universe, V . Start with a ground model V of ZFC and a partially ordered set (P, ≤) ∈ V . Pick an object G ⊂ P where:

◮ G is a filter. ◮ G meets every maximal antichain of P.

This G is called a generic filter of P, and G / ∈ V . Then obtain the model V [G] of ZFC as follows:

◮ A P-name τ in V is a set of the form

{σ, p | σ is a P-name and p ∈ P}.

◮ For each P-name τ in V , set τ G = {σG | (∃p ∈ G)σ, p ∈ τ} ◮ Set V [G] = {τ G | τ is a P-name}.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 56

Using forcing to add new subsets of a cardinal κ

Obtaining consistency results about κ → 2κ is done by forcing to add new subsets of κ. Forcing: Adjoin a new object to the set-theoretic universe, V . Start with a ground model V of ZFC and a partially ordered set (P, ≤) ∈ V . Pick an object G ⊂ P where:

◮ G is a filter. ◮ G meets every maximal antichain of P.

This G is called a generic filter of P, and G / ∈ V . Then obtain the model V [G] of ZFC as follows:

◮ A P-name τ in V is a set of the form

{σ, p | σ is a P-name and p ∈ P}.

◮ For each P-name τ in V , set τ G = {σG | (∃p ∈ G)σ, p ∈ τ} ◮ Set V [G] = {τ G | τ is a P-name}.

Information about V [G] can be obtained while working in V via a relation definable in V , called the forcing relation, “p φ”.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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Using forcing to add new subsets of a cardinal κ

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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Using forcing to add new subsets of a cardinal κ

Forcing to add one new subset of κ:

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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Using forcing to add new subsets of a cardinal κ

Forcing to add one new subset of κ:

Definition

Let κ be a regular cardinal. Conditions in Add(κ, 1) are partial functions f : κ → {0, 1}, with | dom(f )| < κ,

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 60

Using forcing to add new subsets of a cardinal κ

Forcing to add one new subset of κ:

Definition

Let κ be a regular cardinal. Conditions in Add(κ, 1) are partial functions f : κ → {0, 1}, with | dom(f )| < κ, ordered by reverse

  • inclusion. I.e. f1 ≤ f2 if f1 ⊃ f2.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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Using forcing to add new subsets of a cardinal κ

Forcing to add one new subset of κ:

Definition

Let κ be a regular cardinal. Conditions in Add(κ, 1) are partial functions f : κ → {0, 1}, with | dom(f )| < κ, ordered by reverse

  • inclusion. I.e. f1 ≤ f2 if f1 ⊃ f2.

Proposition

Add(κ, 1) is κ - closed and has the κ+ chain condition. So, it preserves cardinals.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 62

Using forcing to add new subsets of a cardinal κ

Forcing to add one new subset of κ:

Definition

Let κ be a regular cardinal. Conditions in Add(κ, 1) are partial functions f : κ → {0, 1}, with | dom(f )| < κ, ordered by reverse

  • inclusion. I.e. f1 ≤ f2 if f1 ⊃ f2.

Proposition

Add(κ, 1) is κ - closed and has the κ+ chain condition. So, it preserves cardinals. Let G be Add(κ, 1)-generic over V , and set f ∗ =

f ∈G f .

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 63

Using forcing to add new subsets of a cardinal κ

Forcing to add one new subset of κ:

Definition

Let κ be a regular cardinal. Conditions in Add(κ, 1) are partial functions f : κ → {0, 1}, with | dom(f )| < κ, ordered by reverse

  • inclusion. I.e. f1 ≤ f2 if f1 ⊃ f2.

Proposition

Add(κ, 1) is κ - closed and has the κ+ chain condition. So, it preserves cardinals. Let G be Add(κ, 1)-generic over V , and set f ∗ =

f ∈G f . Then

f ∗ : κ → {0, 1} is a total function and a =def {α < κ | f ∗(α) = 1} is a new subset of κ. I.e. a ∈ V [G] \ V .

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 64

Using forcing to add new subsets of a cardinal κ

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 65

Using forcing to add new subsets of a cardinal κ

When κ is regular:

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 66

Using forcing to add new subsets of a cardinal κ

When κ is regular: Add(κ, λ) is the Cohen poset to add λ many subsets to κ.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 67

Using forcing to add new subsets of a cardinal κ

When κ is regular: Add(κ, λ) is the Cohen poset to add λ many subsets to κ. Conditions are partial functions f : λ × κ → {0, 1} with | dom(f )| < κ, ordered by reverse inclusion.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 68

Using forcing to add new subsets of a cardinal κ

When κ is regular: Add(κ, λ) is the Cohen poset to add λ many subsets to κ. Conditions are partial functions f : λ × κ → {0, 1} with | dom(f )| < κ, ordered by reverse inclusion.

◮ Add(κ, λ) is κ-closed and has the κ+ chain condition, and so

cardinals are preserved.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 69

Using forcing to add new subsets of a cardinal κ

When κ is regular: Add(κ, λ) is the Cohen poset to add λ many subsets to κ. Conditions are partial functions f : λ × κ → {0, 1} with | dom(f )| < κ, ordered by reverse inclusion.

◮ Add(κ, λ) is κ-closed and has the κ+ chain condition, and so

cardinals are preserved.

◮ Add(κ, λ) adds λ many new subsets of κ.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 70

Using forcing to add new subsets of a cardinal κ

When κ is regular: Add(κ, λ) is the Cohen poset to add λ many subsets to κ. Conditions are partial functions f : λ × κ → {0, 1} with | dom(f )| < κ, ordered by reverse inclusion.

◮ Add(κ, λ) is κ-closed and has the κ+ chain condition, and so

cardinals are preserved.

◮ Add(κ, λ) adds λ many new subsets of κ.

When κ is singular:

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 71

Using forcing to add new subsets of a cardinal κ

When κ is regular: Add(κ, λ) is the Cohen poset to add λ many subsets to κ. Conditions are partial functions f : λ × κ → {0, 1} with | dom(f )| < κ, ordered by reverse inclusion.

◮ Add(κ, λ) is κ-closed and has the κ+ chain condition, and so

cardinals are preserved.

◮ Add(κ, λ) adds λ many new subsets of κ.

When κ is singular:

◮ The above poset will collapse cardinals. So, we need a

different approach.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 72

Using forcing to add new subsets of a cardinal κ

When κ is regular: Add(κ, λ) is the Cohen poset to add λ many subsets to κ. Conditions are partial functions f : λ × κ → {0, 1} with | dom(f )| < κ, ordered by reverse inclusion.

◮ Add(κ, λ) is κ-closed and has the κ+ chain condition, and so

cardinals are preserved.

◮ Add(κ, λ) adds λ many new subsets of κ.

When κ is singular:

◮ The above poset will collapse cardinals. So, we need a

different approach.

◮ One strategy: turn a regular cardinal into a singular.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 73

Using forcing to add new subsets of a cardinal κ

When κ is regular: Add(κ, λ) is the Cohen poset to add λ many subsets to κ. Conditions are partial functions f : λ × κ → {0, 1} with | dom(f )| < κ, ordered by reverse inclusion.

◮ Add(κ, λ) is κ-closed and has the κ+ chain condition, and so

cardinals are preserved.

◮ Add(κ, λ) adds λ many new subsets of κ.

When κ is singular:

◮ The above poset will collapse cardinals. So, we need a

different approach.

◮ One strategy: turn a regular cardinal into a singular. ◮ Prikry forcing: changes cofinality without collapsing cardinals;

requires large cardinals.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 74

Large cardinals

Large cardinal axioms assert the existence of certain “large” cardinals that have strong reflection properties.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 75

Large cardinals

Large cardinal axioms assert the existence of certain “large” cardinals that have strong reflection properties. These axioms provide a strengthening of ZFC.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 76

Large cardinals

Large cardinal axioms assert the existence of certain “large” cardinals that have strong reflection properties. These axioms provide a strengthening of ZFC. The following are some large cardinals in an increasing consistency strength:

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 77

Large cardinals

Large cardinal axioms assert the existence of certain “large” cardinals that have strong reflection properties. These axioms provide a strengthening of ZFC. The following are some large cardinals in an increasing consistency strength:

◮ κ is measurable if there is a normal nonprincipal κ-complete

ultrafilter U on κ. U is also called a normal measure.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 78

Large cardinals

Large cardinal axioms assert the existence of certain “large” cardinals that have strong reflection properties. These axioms provide a strengthening of ZFC. The following are some large cardinals in an increasing consistency strength:

◮ κ is measurable if there is a normal nonprincipal κ-complete

ultrafilter U on κ. U is also called a normal measure.

◮ κ is λ-supercompact if there is a normal nonprincipal

κ-complete ultrafilter on Pκ(λ). U is also called a supercompactness measure on Pκ(λ).

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 79

Large cardinals

Large cardinal axioms assert the existence of certain “large” cardinals that have strong reflection properties. These axioms provide a strengthening of ZFC. The following are some large cardinals in an increasing consistency strength:

◮ κ is measurable if there is a normal nonprincipal κ-complete

ultrafilter U on κ. U is also called a normal measure.

◮ κ is λ-supercompact if there is a normal nonprincipal

κ-complete ultrafilter on Pκ(λ). U is also called a supercompactness measure on Pκ(λ).

◮ κ is supercompact if it is λ-supercompact for all λ.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 80

Large cardinals

Large cardinal axioms assert the existence of certain “large” cardinals that have strong reflection properties. These axioms provide a strengthening of ZFC. The following are some large cardinals in an increasing consistency strength:

◮ κ is measurable if there is a normal nonprincipal κ-complete

ultrafilter U on κ. U is also called a normal measure.

◮ κ is λ-supercompact if there is a normal nonprincipal

κ-complete ultrafilter on Pκ(λ). U is also called a supercompactness measure on Pκ(λ).

◮ κ is supercompact if it is λ-supercompact for all λ.

Remark

An alternative way to define these large cardinals is via elementary embeddings of the set theoretic universe.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 81

Prikry type forcing

Classical Prikry forcing:

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 82

Prikry type forcing

Classical Prikry forcing: Let κ be a measurable cardinal and U be a normal measure on κ.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 83

Prikry type forcing

Classical Prikry forcing: Let κ be a measurable cardinal and U be a normal measure on κ. The forcing conditions are pairs s, A, where s is a finite sequence of ordinals in κ and A ∈ U.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 84

Prikry type forcing

Classical Prikry forcing: Let κ be a measurable cardinal and U be a normal measure on κ. The forcing conditions are pairs s, A, where s is a finite sequence of ordinals in κ and A ∈ U. s1, A1 ≤ s0, A0 iff:

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 85

Prikry type forcing

Classical Prikry forcing: Let κ be a measurable cardinal and U be a normal measure on κ. The forcing conditions are pairs s, A, where s is a finite sequence of ordinals in κ and A ∈ U. s1, A1 ≤ s0, A0 iff:

◮ s0 is an initial segment of s1. ◮ s1 \ s0 ⊂ A0, ◮ A1 ⊂ A0.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 86

Prikry type forcing

Classical Prikry forcing: Let κ be a measurable cardinal and U be a normal measure on κ. The forcing conditions are pairs s, A, where s is a finite sequence of ordinals in κ and A ∈ U. s1, A1 ≤ s0, A0 iff:

◮ s0 is an initial segment of s1. ◮ s1 \ s0 ⊂ A0, ◮ A1 ⊂ A0.

Let G be P-generic over V . Set s∗ = {s | (∃A)s, A ∈ G}; s∗ is an ω-sequence cofinal in κ. And so, in V [G]:

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 87

Prikry type forcing

Classical Prikry forcing: Let κ be a measurable cardinal and U be a normal measure on κ. The forcing conditions are pairs s, A, where s is a finite sequence of ordinals in κ and A ∈ U. s1, A1 ≤ s0, A0 iff:

◮ s0 is an initial segment of s1. ◮ s1 \ s0 ⊂ A0, ◮ A1 ⊂ A0.

Let G be P-generic over V . Set s∗ = {s | (∃A)s, A ∈ G}; s∗ is an ω-sequence cofinal in κ. And so, in V [G]:

◮ cf(κ) = ω,

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 88

Prikry type forcing

Classical Prikry forcing: Let κ be a measurable cardinal and U be a normal measure on κ. The forcing conditions are pairs s, A, where s is a finite sequence of ordinals in κ and A ∈ U. s1, A1 ≤ s0, A0 iff:

◮ s0 is an initial segment of s1. ◮ s1 \ s0 ⊂ A0, ◮ A1 ⊂ A0.

Let G be P-generic over V . Set s∗ = {s | (∃A)s, A ∈ G}; s∗ is an ω-sequence cofinal in κ. And so, in V [G]:

◮ cf(κ) = ω, ◮ V and V [G] have the same cardinals.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 89

Prikry type forcing

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 90

Prikry type forcing

Motivation: blowing up the power set of a singular cardinal in

  • rder to construct models of not SCH.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 91

Prikry type forcing

Motivation: blowing up the power set of a singular cardinal in

  • rder to construct models of not SCH.

◮ Classical Prikry: starts with a normal measure on κ and adds

a cofinal ω-sequence in κ, while preserving cardinals.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 92

Prikry type forcing

Motivation: blowing up the power set of a singular cardinal in

  • rder to construct models of not SCH.

◮ Classical Prikry: starts with a normal measure on κ and adds

a cofinal ω-sequence in κ, while preserving cardinals.

◮ Violating SCH: Let κ be a Laver indestructible supercompact

cardinal.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 93

Prikry type forcing

Motivation: blowing up the power set of a singular cardinal in

  • rder to construct models of not SCH.

◮ Classical Prikry: starts with a normal measure on κ and adds

a cofinal ω-sequence in κ, while preserving cardinals.

◮ Violating SCH: Let κ be a Laver indestructible supercompact

cardinal.

◮ Force to add κ++ many subsets of κ. Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 94

Prikry type forcing

Motivation: blowing up the power set of a singular cardinal in

  • rder to construct models of not SCH.

◮ Classical Prikry: starts with a normal measure on κ and adds

a cofinal ω-sequence in κ, while preserving cardinals.

◮ Violating SCH: Let κ be a Laver indestructible supercompact

cardinal.

◮ Force to add κ++ many subsets of κ. ◮ Then force with Prikry forcing to make κ have cofinality ω. Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 95

Prikry type forcing

Motivation: blowing up the power set of a singular cardinal in

  • rder to construct models of not SCH.

◮ Classical Prikry: starts with a normal measure on κ and adds

a cofinal ω-sequence in κ, while preserving cardinals.

◮ Violating SCH: Let κ be a Laver indestructible supercompact

cardinal.

◮ Force to add κ++ many subsets of κ. ◮ Then force with Prikry forcing to make κ have cofinality ω.

In the final model cardinals are preserved, κ remains strong limit, and 2κ > κ+. I.e. SCH fails at κ.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 96

Prikry type forcing

The following are some variations:

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 97

Prikry type forcing

The following are some variations:

  • 1. Supercompact Prikry:

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 98

Prikry type forcing

The following are some variations:

  • 1. Supercompact Prikry:

◮ start with a supercompactness measure U on Pκ(η); Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 99

Prikry type forcing

The following are some variations:

  • 1. Supercompact Prikry:

◮ start with a supercompactness measure U on Pκ(η); ◮ force to add an increasing ω-sequence of sets xn ∈ (Pκ(η))V ,

with η =

n xn.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 100

Prikry type forcing

The following are some variations:

  • 1. Supercompact Prikry:

◮ start with a supercompactness measure U on Pκ(η); ◮ force to add an increasing ω-sequence of sets xn ∈ (Pκ(η))V ,

with η =

n xn.

  • 2. Gitik-Sharon’s diagonal supercompact Prikry:

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 101

Prikry type forcing

The following are some variations:

  • 1. Supercompact Prikry:

◮ start with a supercompactness measure U on Pκ(η); ◮ force to add an increasing ω-sequence of sets xn ∈ (Pκ(η))V ,

with η =

n xn.

  • 2. Gitik-Sharon’s diagonal supercompact Prikry:

◮ start with a sequence Un | n < ω of supercompactness

measures on Pκ(κ+n);

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 102

Prikry type forcing

The following are some variations:

  • 1. Supercompact Prikry:

◮ start with a supercompactness measure U on Pκ(η); ◮ force to add an increasing ω-sequence of sets xn ∈ (Pκ(η))V ,

with η =

n xn.

  • 2. Gitik-Sharon’s diagonal supercompact Prikry:

◮ start with a sequence Un | n < ω of supercompactness

measures on Pκ(κ+n);

◮ force to add an increasing ω-sequence of sets xn ∈ Pκ((κ+n)V )

with (κ+ω)V =

n xn.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 103

Prikry type forcing

The following are some variations:

  • 1. Supercompact Prikry:

◮ start with a supercompactness measure U on Pκ(η); ◮ force to add an increasing ω-sequence of sets xn ∈ (Pκ(η))V ,

with η =

n xn.

  • 2. Gitik-Sharon’s diagonal supercompact Prikry:

◮ start with a sequence Un | n < ω of supercompactness

measures on Pκ(κ+n);

◮ force to add an increasing ω-sequence of sets xn ∈ Pκ((κ+n)V )

with (κ+ω)V =

n xn.

The strategy: add subsets to a large cardinal, then singularize it.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 104

Extender based forcing

Alternative way: start with a singular κ; say κ = supn κn; and blow up its powerset to some regular λ in a Prikry fashion via extender based forcing.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 105

Extender based forcing

Alternative way: start with a singular κ; say κ = supn κn; and blow up its powerset to some regular λ in a Prikry fashion via extender based forcing.

◮ Developed by Gitik-Magidor.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 106

Extender based forcing

Alternative way: start with a singular κ; say κ = supn κn; and blow up its powerset to some regular λ in a Prikry fashion via extender based forcing.

◮ Developed by Gitik-Magidor. ◮ Adds λ sequences through n κn, and so 2κ becomes λ.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 107

Extender based forcing

Alternative way: start with a singular κ; say κ = supn κn; and blow up its powerset to some regular λ in a Prikry fashion via extender based forcing.

◮ Developed by Gitik-Magidor. ◮ Adds λ sequences through n κn, and so 2κ becomes λ. ◮ Recall: adding one Prikry sequence requires an ultrafilter.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 108

Extender based forcing

Alternative way: start with a singular κ; say κ = supn κn; and blow up its powerset to some regular λ in a Prikry fashion via extender based forcing.

◮ Developed by Gitik-Magidor. ◮ Adds λ sequences through n κn, and so 2κ becomes λ. ◮ Recall: adding one Prikry sequence requires an ultrafilter.

Here, we need many ultrafilters.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 109

Extender based forcing

Alternative way: start with a singular κ; say κ = supn κn; and blow up its powerset to some regular λ in a Prikry fashion via extender based forcing.

◮ Developed by Gitik-Magidor. ◮ Adds λ sequences through n κn, and so 2κ becomes λ. ◮ Recall: adding one Prikry sequence requires an ultrafilter.

Here, we need many ultrafilters.

◮ In particular, this forcing uses extenders;

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

slide-110
SLIDE 110

Extender based forcing

Alternative way: start with a singular κ; say κ = supn κn; and blow up its powerset to some regular λ in a Prikry fashion via extender based forcing.

◮ Developed by Gitik-Magidor. ◮ Adds λ sequences through n κn, and so 2κ becomes λ. ◮ Recall: adding one Prikry sequence requires an ultrafilter.

Here, we need many ultrafilters.

◮ In particular, this forcing uses extenders; an extender is a

system of ultrafilters.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

slide-111
SLIDE 111

Extender based forcing

Alternative way: start with a singular κ; say κ = supn κn; and blow up its powerset to some regular λ in a Prikry fashion via extender based forcing.

◮ Developed by Gitik-Magidor. ◮ Adds λ sequences through n κn, and so 2κ becomes λ. ◮ Recall: adding one Prikry sequence requires an ultrafilter.

Here, we need many ultrafilters.

◮ In particular, this forcing uses extenders; an extender is a

system of ultrafilters.

◮ No need to add subsets of κ in advance, so can keep GCH

below κ, as opposed to the above forcings.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 112

Two general strategies to blow up the powerset of a singular cardinal

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 113

Two general strategies to blow up the powerset of a singular cardinal

  • 1. Add Cohen subsets to a large cardinal κ.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 114

Two general strategies to blow up the powerset of a singular cardinal

  • 1. Add Cohen subsets to a large cardinal κ. Then singularize it.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 115

Two general strategies to blow up the powerset of a singular cardinal

  • 1. Add Cohen subsets to a large cardinal κ. Then singularize it.

◮ By the reflection properties of κ, also have to add subsets to

many α’s below κ.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 116

Two general strategies to blow up the powerset of a singular cardinal

  • 1. Add Cohen subsets to a large cardinal κ. Then singularize it.

◮ By the reflection properties of κ, also have to add subsets to

many α’s below κ.

◮ So, in the final model κ is strong limit, but GCH below κ fails. Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

slide-117
SLIDE 117

Two general strategies to blow up the powerset of a singular cardinal

  • 1. Add Cohen subsets to a large cardinal κ. Then singularize it.

◮ By the reflection properties of κ, also have to add subsets to

many α’s below κ.

◮ So, in the final model κ is strong limit, but GCH below κ fails.

  • 2. Start with a singular κ;

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

slide-118
SLIDE 118

Two general strategies to blow up the powerset of a singular cardinal

  • 1. Add Cohen subsets to a large cardinal κ. Then singularize it.

◮ By the reflection properties of κ, also have to add subsets to

many α’s below κ.

◮ So, in the final model κ is strong limit, but GCH below κ fails.

  • 2. Start with a singular κ; κ =

n κn, where each κn is large.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

slide-119
SLIDE 119

Two general strategies to blow up the powerset of a singular cardinal

  • 1. Add Cohen subsets to a large cardinal κ. Then singularize it.

◮ By the reflection properties of κ, also have to add subsets to

many α’s below κ.

◮ So, in the final model κ is strong limit, but GCH below κ fails.

  • 2. Start with a singular κ; κ =

n κn, where each κn is large.

Then add many Prikry sequences through

n κn.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

slide-120
SLIDE 120

Two general strategies to blow up the powerset of a singular cardinal

  • 1. Add Cohen subsets to a large cardinal κ. Then singularize it.

◮ By the reflection properties of κ, also have to add subsets to

many α’s below κ.

◮ So, in the final model κ is strong limit, but GCH below κ fails.

  • 2. Start with a singular κ; κ =

n κn, where each κn is large.

Then add many Prikry sequences through

n κn.

◮ Here, in the final model GCH below κ holds. Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

slide-121
SLIDE 121

Two general strategies to blow up the powerset of a singular cardinal

  • 1. Add Cohen subsets to a large cardinal κ. Then singularize it.

◮ By the reflection properties of κ, also have to add subsets to

many α’s below κ.

◮ So, in the final model κ is strong limit, but GCH below κ fails.

  • 2. Start with a singular κ; κ =

n κn, where each κn is large.

Then add many Prikry sequences through

n κn.

◮ Here, in the final model GCH below κ holds.

Advantage of the first strategy:

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 122

Two general strategies to blow up the powerset of a singular cardinal

  • 1. Add Cohen subsets to a large cardinal κ. Then singularize it.

◮ By the reflection properties of κ, also have to add subsets to

many α’s below κ.

◮ So, in the final model κ is strong limit, but GCH below κ fails.

  • 2. Start with a singular κ; κ =

n κn, where each κn is large.

Then add many Prikry sequences through

n κn.

◮ Here, in the final model GCH below κ holds.

Advantage of the first strategy: Can singularize/collapse an interval of cardinals above κ, that gives more freedom in obtaining consistency results about combinatorial properties such as scales.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

slide-123
SLIDE 123

Two general strategies to blow up the powerset of a singular cardinal

  • 1. Add Cohen subsets to a large cardinal κ. Then singularize it.

◮ By the reflection properties of κ, also have to add subsets to

many α’s below κ.

◮ So, in the final model κ is strong limit, but GCH below κ fails.

  • 2. Start with a singular κ; κ =

n κn, where each κn is large.

Then add many Prikry sequences through

n κn.

◮ Here, in the final model GCH below κ holds.

Advantage of the first strategy: Can singularize/collapse an interval of cardinals above κ, that gives more freedom in obtaining consistency results about combinatorial properties such as scales. But lose GCH below κ.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 124

The hybrid Prikry

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 125

The hybrid Prikry

Question: can we combine the advantages of the first strategy with the method of the second strategy, in order to maintain GCH below κ?

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 126

The hybrid Prikry

Question: can we combine the advantages of the first strategy with the method of the second strategy, in order to maintain GCH below κ? Motivation: obtaining consistency results about combinatorial principles like square and failure of SCH, but keeping GCH below κ.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 127

The hybrid Prikry

Question: can we combine the advantages of the first strategy with the method of the second strategy, in order to maintain GCH below κ? Motivation: obtaining consistency results about combinatorial principles like square and failure of SCH, but keeping GCH below κ.

Theorem

(S.) Starting from a supercompact cardinal κ, there is a forcing which simultaneously singularizes κ and increases its powerset, while maintaining GCH below κ.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 128

The hybrid Prikry

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 129

The hybrid Prikry

Definition: Hybrid Prikry: (S.) Suppose that κ is supercompact and GCH holds. There is a Prikry type forcing notion, P, that simultaneously singularizes a supercompact κ and adds many subsets to it.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 130

The hybrid Prikry

Definition: Hybrid Prikry: (S.) Suppose that κ is supercompact and GCH holds. There is a Prikry type forcing notion, P, that simultaneously singularizes a supercompact κ and adds many subsets to it.

◮ P combines extender based forcing with diagonal

supercompact Prikry.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 131

The hybrid Prikry

Definition: Hybrid Prikry: (S.) Suppose that κ is supercompact and GCH holds. There is a Prikry type forcing notion, P, that simultaneously singularizes a supercompact κ and adds many subsets to it.

◮ P combines extender based forcing with diagonal

supercompact Prikry.

◮ The κn’s will be chosen generically.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

slide-132
SLIDE 132

The hybrid Prikry

Definition: Hybrid Prikry: (S.) Suppose that κ is supercompact and GCH holds. There is a Prikry type forcing notion, P, that simultaneously singularizes a supercompact κ and adds many subsets to it.

◮ P combines extender based forcing with diagonal

supercompact Prikry.

◮ The κn’s will be chosen generically. ◮ No bounded subsets of κ are added.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

slide-133
SLIDE 133

The hybrid Prikry

Definition: Hybrid Prikry: (S.) Suppose that κ is supercompact and GCH holds. There is a Prikry type forcing notion, P, that simultaneously singularizes a supercompact κ and adds many subsets to it.

◮ P combines extender based forcing with diagonal

supercompact Prikry.

◮ The κn’s will be chosen generically. ◮ No bounded subsets of κ are added. ◮ In the final model, GCH holds below κ, and 2κ > κ+. So SCH

fails at κ.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

slide-134
SLIDE 134

The hybrid Prikry

Definition: Hybrid Prikry: (S.) Suppose that κ is supercompact and GCH holds. There is a Prikry type forcing notion, P, that simultaneously singularizes a supercompact κ and adds many subsets to it.

◮ P combines extender based forcing with diagonal

supercompact Prikry.

◮ The κn’s will be chosen generically. ◮ No bounded subsets of κ are added. ◮ In the final model, GCH holds below κ, and 2κ > κ+. So SCH

fails at κ.

◮ Collapses κ+ and actually an interval of cardinals (unlike the

classical extender based forcing).

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 135

Square principles

◮ Isolated by Jensen in his fine structure analysis of L.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 136

Square principles

◮ Isolated by Jensen in his fine structure analysis of L. ◮ κ states that there is a coherent sequence of closed and

unbounded sets singularizing ordinals α < κ+.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 137

Square principles

◮ Isolated by Jensen in his fine structure analysis of L. ◮ κ states that there is a coherent sequence of closed and

unbounded sets singularizing ordinals α < κ+. There is Cα | α < κ+, s.t.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 138

Square principles

◮ Isolated by Jensen in his fine structure analysis of L. ◮ κ states that there is a coherent sequence of closed and

unbounded sets singularizing ordinals α < κ+. There is Cα | α < κ+, s.t.

◮ each Cα is club in α of order type ≤ κ, and Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 139

Square principles

◮ Isolated by Jensen in his fine structure analysis of L. ◮ κ states that there is a coherent sequence of closed and

unbounded sets singularizing ordinals α < κ+. There is Cα | α < κ+, s.t.

◮ each Cα is club in α of order type ≤ κ, and ◮ if β is a limit point of Cα, then Cα ∩ β = Cβ. Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 140

Square principles

◮ Isolated by Jensen in his fine structure analysis of L. ◮ κ states that there is a coherent sequence of closed and

unbounded sets singularizing ordinals α < κ+. There is Cα | α < κ+, s.t.

◮ each Cα is club in α of order type ≤ κ, and ◮ if β is a limit point of Cα, then Cα ∩ β = Cβ.

◮ ∗ κ is a weakening which allows up to κ guesses for each club.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 141

Square principles

◮ Isolated by Jensen in his fine structure analysis of L. ◮ κ states that there is a coherent sequence of closed and

unbounded sets singularizing ordinals α < κ+. There is Cα | α < κ+, s.t.

◮ each Cα is club in α of order type ≤ κ, and ◮ if β is a limit point of Cα, then Cα ∩ β = Cβ.

◮ ∗ κ is a weakening which allows up to κ guesses for each club. ◮ κ<κ = κ → ∗ κ; so we focus on the case κ singular.

Lemma

In the Hybrid Prikry model, we have ∗

κ.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 142

Scales

Let κ = supn<ω κn, where every κn is a regular cardinal.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 143

Scales

Let κ = supn<ω κn, where every κn is a regular cardinal. For f and g in

n<ω κn, we say that f <∗ g if f (n) < g(n) for all

large n.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 144

Scales

Let κ = supn<ω κn, where every κn is a regular cardinal. For f and g in

n<ω κn, we say that f <∗ g if f (n) < g(n) for all

large n. A scale of length µ is a sequence of functions fα | α < µ from

  • n<ω κn which is increasing and cofinal with respect to <∗.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 145

Scales

Let κ = supn<ω κn, where every κn is a regular cardinal. For f and g in

n<ω κn, we say that f <∗ g if f (n) < g(n) for all

large n. A scale of length µ is a sequence of functions fα | α < µ from

  • n<ω κn which is increasing and cofinal with respect to <∗.

A point γ < µ of cofinality between ω and κ is a good point iff

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 146

Scales

Let κ = supn<ω κn, where every κn is a regular cardinal. For f and g in

n<ω κn, we say that f <∗ g if f (n) < g(n) for all

large n. A scale of length µ is a sequence of functions fα | α < µ from

  • n<ω κn which is increasing and cofinal with respect to <∗.

A point γ < µ of cofinality between ω and κ is a good point iff there exists an unbounded A ⊆ γ, such that fα(n) | α ∈ A is strictly increasing for all large n.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 147

Scales

Let κ = supn<ω κn, where every κn is a regular cardinal. For f and g in

n<ω κn, we say that f <∗ g if f (n) < g(n) for all

large n. A scale of length µ is a sequence of functions fα | α < µ from

  • n<ω κn which is increasing and cofinal with respect to <∗.

A point γ < µ of cofinality between ω and κ is a good point iff there exists an unbounded A ⊆ γ, such that fα(n) | α ∈ A is strictly increasing for all large n. If A is club in γ, then γ is a very good point.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

slide-148
SLIDE 148

Scales

Let κ = supn<ω κn, where every κn is a regular cardinal. For f and g in

n<ω κn, we say that f <∗ g if f (n) < g(n) for all

large n. A scale of length µ is a sequence of functions fα | α < µ from

  • n<ω κn which is increasing and cofinal with respect to <∗.

A point γ < µ of cofinality between ω and κ is a good point iff there exists an unbounded A ⊆ γ, such that fα(n) | α ∈ A is strictly increasing for all large n. If A is club in γ, then γ is a very good point. A scale is (very) good iff modulo the club filter on µ, almost every point of cofinality between cf(κ) and κ is (very) good.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 149

Scales

Let κ = supn<ω κn, where every κn is a regular cardinal. For f and g in

n<ω κn, we say that f <∗ g if f (n) < g(n) for all

large n. A scale of length µ is a sequence of functions fα | α < µ from

  • n<ω κn which is increasing and cofinal with respect to <∗.

A point γ < µ of cofinality between ω and κ is a good point iff there exists an unbounded A ⊆ γ, such that fα(n) | α ∈ A is strictly increasing for all large n. If A is club in γ, then γ is a very good point. A scale is (very) good iff modulo the club filter on µ, almost every point of cofinality between cf(κ) and κ is (very) good.

Lemma

When forcing with Hybrid Prikry, scales in

n κ+n+1 from V

generate scales

n κ in the generic extension.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 150

Combinatorial principles, continued

  • 1. → ∗ → all scales are good.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 151

Combinatorial principles, continued

  • 1. → ∗ → all scales are good.
  • 2. There are no good scales above a supercompact.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 152

Combinatorial principles, continued

  • 1. → ∗ → all scales are good.
  • 2. There are no good scales above a supercompact.

And square principles fail above a supercompact.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 153

Combinatorial principles, continued

  • 1. → ∗ → all scales are good.
  • 2. There are no good scales above a supercompact.

And square principles fail above a supercompact. More precisely, if κ is supercompact, cf(ν) < κ < ν, there are no good scales at ν ( and so ∗ also fails).

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 154

Combinatorial principles, continued

  • 1. → ∗ → all scales are good.
  • 2. There are no good scales above a supercompact.

And square principles fail above a supercompact. More precisely, if κ is supercompact, cf(ν) < κ < ν, there are no good scales at ν ( and so ∗ also fails).

  • 3. ∗

κ → VGSκ.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 155

Combinatorial principles, continued

  • 1. → ∗ → all scales are good.
  • 2. There are no good scales above a supercompact.

And square principles fail above a supercompact. More precisely, if κ is supercompact, cf(ν) < κ < ν, there are no good scales at ν ( and so ∗ also fails).

  • 3. ∗

κ → VGSκ.

  • 4. VGSκ → ∗

κ.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 156

Not SCH and Very good scales

Question: Does ¬SCHκ imply a very good scale at κ?

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 157

Not SCH and Very good scales

Question: Does ¬SCHκ imply a very good scale at κ? Some motivation:

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

slide-158
SLIDE 158

Not SCH and Very good scales

Question: Does ¬SCHκ imply a very good scale at κ? Some motivation:

◮ Let P be the classical Prikry.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 159

Not SCH and Very good scales

Question: Does ¬SCHκ imply a very good scale at κ? Some motivation:

◮ Let P be the classical Prikry.

Forcing with Add(κ, κ++) ∗ P gives:

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 160

Not SCH and Very good scales

Question: Does ¬SCHκ imply a very good scale at κ? Some motivation:

◮ Let P be the classical Prikry.

Forcing with Add(κ, κ++) ∗ P gives:

◮ κ is strong limit, 2κ = κ++, and so ¬SCHκ Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 161

Not SCH and Very good scales

Question: Does ¬SCHκ imply a very good scale at κ? Some motivation:

◮ Let P be the classical Prikry.

Forcing with Add(κ, κ++) ∗ P gives:

◮ κ is strong limit, 2κ = κ++, and so ¬SCHκ ◮ there is a very good scale at κ of length κ++. Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

slide-162
SLIDE 162

Not SCH and Very good scales

Question: Does ¬SCHκ imply a very good scale at κ? Some motivation:

◮ Let P be the classical Prikry.

Forcing with Add(κ, κ++) ∗ P gives:

◮ κ is strong limit, 2κ = κ++, and so ¬SCHκ ◮ there is a very good scale at κ of length κ++.

◮ Let P[κ,<µ) be Prikry forcing singularizing everything in the

interval [κ, < µ).

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

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SLIDE 163

Not SCH and Very good scales

Question: Does ¬SCHκ imply a very good scale at κ? Some motivation:

◮ Let P be the classical Prikry.

Forcing with Add(κ, κ++) ∗ P gives:

◮ κ is strong limit, 2κ = κ++, and so ¬SCHκ ◮ there is a very good scale at κ of length κ++.

◮ Let P[κ,<µ) be Prikry forcing singularizing everything in the

interval [κ, < µ). Forcing with Add(κ, µ+) ∗ Pκ,<µ gives same as above.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

slide-164
SLIDE 164

Not SCH and Very good scales

Question: Does ¬SCHκ imply a very good scale at κ? Some motivation:

◮ Let P be the classical Prikry.

Forcing with Add(κ, κ++) ∗ P gives:

◮ κ is strong limit, 2κ = κ++, and so ¬SCHκ ◮ there is a very good scale at κ of length κ++.

◮ Let P[κ,<µ) be Prikry forcing singularizing everything in the

interval [κ, < µ). Forcing with Add(κ, µ+) ∗ Pκ,<µ gives same as above.

Theorem

(S.) It is consistent to have κ strong limit, 2κ = κ++, and so ¬SCHκ and no very good scale at κ

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

slide-165
SLIDE 165

Not SCH and Very good scales

Question: Does ¬SCHκ imply a very good scale at κ? Some motivation:

◮ Let P be the classical Prikry.

Forcing with Add(κ, κ++) ∗ P gives:

◮ κ is strong limit, 2κ = κ++, and so ¬SCHκ ◮ there is a very good scale at κ of length κ++.

◮ Let P[κ,<µ) be Prikry forcing singularizing everything in the

interval [κ, < µ). Forcing with Add(κ, µ+) ∗ Pκ,<µ gives same as above.

Theorem

(S.) It is consistent to have κ strong limit, 2κ = κ++, and so ¬SCHκ and no very good scale at κ The proof uses a variation of the Hybrid Prikry.

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

slide-166
SLIDE 166

Not SCH and Very good scales

Question: Does ¬SCHκ imply a very good scale at κ? Some motivation:

◮ Let P be the classical Prikry.

Forcing with Add(κ, κ++) ∗ P gives:

◮ κ is strong limit, 2κ = κ++, and so ¬SCHκ ◮ there is a very good scale at κ of length κ++.

◮ Let P[κ,<µ) be Prikry forcing singularizing everything in the

interval [κ, < µ). Forcing with Add(κ, µ+) ∗ Pκ,<µ gives same as above.

Theorem

(S.) It is consistent to have κ strong limit, 2κ = κ++, and so ¬SCHκ and no very good scale at κ The proof uses a variation of the Hybrid Prikry. Question: can we also get the above with no very good scale of length κ+?

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals

slide-167
SLIDE 167

Not SCH and Very good scales

Question: Does ¬SCHκ imply a very good scale at κ? Some motivation:

◮ Let P be the classical Prikry.

Forcing with Add(κ, κ++) ∗ P gives:

◮ κ is strong limit, 2κ = κ++, and so ¬SCHκ ◮ there is a very good scale at κ of length κ++.

◮ Let P[κ,<µ) be Prikry forcing singularizing everything in the

interval [κ, < µ). Forcing with Add(κ, µ+) ∗ Pκ,<µ gives same as above.

Theorem

(S.) It is consistent to have κ strong limit, 2κ = κ++, and so ¬SCHκ and no very good scale at κ The proof uses a variation of the Hybrid Prikry. Question: can we also get the above with no very good scale of length κ+?

Dima Sinapova University of Illinois at Chicago Combinatorial properties of singular cardinals