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import Mathlib
import OAI.SetTheory.PartitionConsistency.Models.ClassFibers
import OAI.SetTheory.PartitionConsistency.Forcing.ChoiceFailure
namespace OAI
/-! ## Antichain -/
namespace PartitionConsistency.ForcingQuotient
universe u
noncomputable section
variable {P : Type u} [Preorder P]
/-- Every set of forcing conditions has a maximal incompatible subfamily.
The conclusion is predensity in that set; no cardinal chain condition is used. -/
theorem maximal_antichain (D : Set P) :
∃ A : Set P, A ⊆ D ∧
(∀ p ∈ A, ∀ q ∈ A, ∀ r, r ≤ p → r ≤ q → p = q) ∧
∀ d ∈ D, ∃ a ∈ A, ∃ r, r ≤ d ∧ r ≤ a := by
classical
let C : Set (Set P) := {A | A ⊆ D ∧
∀ p ∈ A, ∀ q ∈ A, ∀ r, r ≤ p → r ≤ q → p = q}
obtain ⟨A,hA,hmax⟩ := zorn_subset C (by
intro c hc hchain
refine ⟨⋃₀ c,⟨?_,?_⟩,fun s hs => Set.subset_sUnion_of_mem hs⟩
· rintro p ⟨B,hB,hpB⟩
exact (hc hB).1 hpB
· rintro p ⟨B,hB,hpB⟩ q ⟨C,hC,hqC⟩ r hrp hrq
rcases hchain.total hB hC with hBC | hCB
· exact (hc hC).2 p (hBC hpB) q hqC r hrp hrq
· exact (hc hB).2 p hpB q (hCB hqC) r hrp hrq)
refine ⟨A,hA.1,hA.2,?_⟩
intro d hd
by_contra hn
have hdA : d ∉ A := by
intro h
exact hn ⟨d,h,d,le_rfl,le_rfl⟩
have hi : insert d A ∈ C := by
refine ⟨Set.insert_subset hd hA.1,?_⟩
intro p hp q hq r hrp hrq
rcases hp with rfl | hp <;> rcases hq with rfl | hq
· rfl
· exact False.elim (hn ⟨q,hq,r,hrp,hrq⟩)
· exact False.elim (hn ⟨p,hp,r,hrq,hrp⟩)
· exact hA.2 p hp q hq r hrp hrq
exact hdA (hmax hi (Set.subset_insert _ _) (Set.mem_insert _ _))
end
end PartitionConsistency.ForcingQuotient
/-! ## Maximum -/
namespace PartitionConsistency.ProductForcing
universe u
open SetForcingNames SetForcingNames.SymmetricSystem DiagramForcing
noncomputable section
variable {M I κ K : Type u} [LeftCancelMonoid M] [DiagramOrder.IsConical M]
variable {μ : Cardinal.{u}} (hμ : Cardinal.aleph0 ≤ μ)
/-- The local maximum principle furnished by root probes. Unlike the ordinary
maximum principle, the conclusion has a specified literal supporting diagram,
chosen before the witness. The name is a mixture over a Cohen antichain. -/
theorem localized_maximum [Infinite M] [Infinite I] [Uncountable K]
(hcard : Cardinal.mk M = μ) (hsize : Cardinal.mk M < Cardinal.mk I)
(hmerger : HasFiniteMergers M) (e : M)
(he : Cardinal.mk ((Set.range (fun x : M => e * x))ᶜ : Set M) = Cardinal.mk M)
(hprobes : RootProbes e K)
{n} (φ : Formula (n+1)) (v : Fin n → (system (M := M) (I := I) (κ := κ) hμ).Name)
(p q : Diagram M I) (hq : q.sub e = p)
(hv : ∀ π ∈ SupportFilter.Fix p.range, ∀ i, π • v i = v i)
(d₀ : CohenForcing.Condition I κ) (hd₀ : d₀.support ⊆ q.range)
(hf : (system hμ).Forces v ((d₀,p) : Poset M I κ) φ.ex) :
∃ ν : (system (M := M) (I := I) (κ := κ) hμ).Name,
(∀ π ∈ SupportFilter.Fix q.range, π • ν = ν) ∧
(system hμ).Forces (Fin.snoc v ν) ((d₀,q) : Poset M I κ) φ := by
classical
let S := system (M := M) (I := I) (κ := κ) hμ
have : Nonempty (Diagram M I) := ⟨p⟩
let D : Set (CohenForcing.Condition I κ) := {a | a ≤ d₀ ∧ a.support ⊆ q.range ∧
∃ ν : S.Name, (∀ π ∈ SupportFilter.Fix q.range, π • ν = ν) ∧
S.Forces (Fin.snoc v ν) ((a,q) : Poset M I κ) φ}
obtain ⟨A,hAD,hanti,hpred⟩ := ForcingQuotient.maximal_antichain D
have hchoose : ∀ a : A, ∃ ν : S.Name,
(∀ π ∈ SupportFilter.Fix q.range, π • ν = ν) ∧
S.Forces (Fin.snoc v ν) ((a.val,q) : Poset M I κ) φ :=
fun a => (hAD a.property).2.2
choose f hfix hforce using hchoose
let act : A → Poset M I κ := fun a => ((a.val,q) : Condition M I κ)
let H := SupportFilter.Fix q.range
have hH : H ∈ S.filter := ⟨q.range,by rw [Diagram.cardinal_range,hcard],le_rfl⟩
have hact : ∀ π ∈ H, ∀ a, S.move π (act a) = act a := by
intro π hπ a
have hfixπ := (SupportFilter.mem_Fix _ _).mp hπ
change S.move π ((a.val,q) : Poset M I κ) = ((a.val,q) : Poset M I κ)
rw [move_coe]
apply congrArg WithTop.some
apply Prod.ext
· exact CohenForcing.Condition.permute_eq_of_fixes_support π a.val
(fun j hj => hfixπ j ((hAD a.property).2.1 hj))
· exact Diagram.permute_eq_of_fixes_range π q hfixπ
have hcoh : ∀ i j r, r ≤ act i → r ≤ act j → S.atomic.EqF r (f i) (f j) := by
intro i j r hri hrj
obtain ⟨r₀,hr₀⟩ := exists_condition_below r
have hij : i = j := Subtype.ext (hanti _ i.property _ j.property r₀.1
(WithTop.coe_le_coe.mp (hr₀.trans hri)).1
(WithTop.coe_le_coe.mp (hr₀.trans hrj)).1)
subst j
exact S.atomic.eq_refl _ _
let ν := S.mix f act H hH (fun π hπ a => hfix a π hπ) hact
refine ⟨ν,S.mix_fixed f act H hH _ hact,?_⟩
apply S.atomic.forceFormula_of_dense S.atomic_regular
intro t ht
obtain ⟨t₀,ht₀⟩ := exists_condition_below t
have htd : t₀.1 ≤ d₀ := (WithTop.coe_le_coe.mp (ht₀.trans ht)).1
have htq : t₀.2 ≤ q := (WithTop.coe_le_coe.mp (ht₀.trans ht)).2
let c := t₀.1.restrict q.range
have hcd : c ≤ d₀ := by
intro z hz
exact ⟨htd hz,hd₀ ((CohenForcing.Condition.mem_support _ _).mpr ⟨z.1.2,z.2,hz⟩)⟩
obtain ⟨d,hdc,hds,νd,hfixd,hforced⟩ := localized_existential hμ hcard hsize hmerger e he hprobes
φ v p q hq hv d₀ hf c hcd (t₀.1.support_restrict_subset _)
have hdD : d ∈ D := ⟨hdc.trans hcd,hds,νd,hfixd,hforced⟩
obtain ⟨a,ha,b,hbd,hba⟩ := hpred d hdD
let b' := b.restrict q.range
have hbc : b' ≤ c := by
intro z hz
exact ⟨hbd (hdc hz),hz.2⟩
have hba' : b' ≤ a := by
intro z hz
exact ⟨hba hz,(hAD ha).2.1 ((CohenForcing.Condition.mem_support _ _).mpr ⟨z.1.2,z.2,hz⟩)⟩
have htcomp : CohenForcing.Condition.Compatible t₀.1 b' := by
intro z x y hx hy
exact b'.functional z x y (hbc ⟨hx,hy.2⟩) hy
obtain ⟨s,hst,hsb⟩ := CohenForcing.Condition.compatible_iff.mp htcomp
let a' : A := ⟨a,ha⟩
have hsa : ((s,t₀.2) : Poset M I κ) ≤ act a' :=
WithTop.coe_le_coe.mpr ⟨hsb.trans hba',htq⟩
have heq := S.atomic.eq_mono hsa (S.eq_mix_at f act H hH (fun π hπ a => hfix a π hπ) hact hcoh a')
refine ⟨((s,t₀.2) : Poset M I κ),
(WithTop.coe_le_coe.mpr (show (s,t₀.2) ≤ t₀ from ⟨hst,le_rfl⟩)).trans ht₀,?_⟩
exact (S.forces_snoc_congr φ v heq).mpr (S.atomic.forceFormula_mono hsa (hforce a'))
end
end PartitionConsistency.ProductForcing
/-! ## ChoiceFamily -/
namespace PartitionConsistency.SetLanguage
/-- Auxiliary formula for a value selected from the set `F(i)`.
Its variables are the family graph, the index, and the selected value. -/
def familyMember : Formula 3 :=
.ex ((edge 0 1 3).conj (.mem 2 3))
end PartitionConsistency.SetLanguage
namespace PartitionConsistency.SetForcingNames.SymmetricSystem
universe u v w
noncomputable section
variable {P : Type w} [Preorder P] {Γ : Type v} [Group Γ]
variable (S : SymmetricSystem.{u} P Γ)
theorem forces_nonemptyFamily {n} (v : Fin n → S.Name) (p : P) (F d : Fin n) :
S.Forces v p (SetLanguage.nonemptyFamily F d) ↔
S.Forces ![v F,v d] p (SetLanguage.functionOn 0 1) ∧
∀ x y : S.Name, ∀ q, q ≤ p → S.atomic.MemF q x (v d) →
∀ r, r ≤ q → S.App r (v F) x y →
∀ s, s ≤ r → ∃ t, t ≤ s ∧ ∃ z : S.Name, S.atomic.MemF t z y := by
simp only [Forces,SetLanguage.nonemptyFamily,S.atomic.forceFormula_rename S.atomic_regular,
S.atomic.forceFormula_all S.atomic_regular,S.atomic.forceFormula_imp S.atomic_regular,
ForcingQuotient.AtomicData.forceFormula_conj,ForcingQuotient.AtomicData.forceFormula_mem,
S.forces_edge,S.forces_nonempty]
have hv : v ∘ ![F,d] = ![v F,v d] := by
ext i
fin_cases i <;> rfl
simp [hv,Fin.snoc]
theorem forces_choiceForFamily {n} (v : Fin n → S.Name) (p : P) (c d F : Fin n) :
S.Forces v p (SetLanguage.choiceForFamily c d F) ↔
S.Forces ![v c,v d] p (SetLanguage.functionOn 0 1) ∧
∀ x y : S.Name, ∀ q, q ≤ p → S.atomic.MemF q x (v d) →
∀ r, r ≤ q → S.App r (v F) x y →
∀ s, s ≤ r → ∃ t, t ≤ s ∧ ∃ z : S.Name,
S.App t (v c) x z ∧ S.atomic.MemF t z y := by
simp only [Forces,SetLanguage.choiceForFamily,S.atomic.forceFormula_rename S.atomic_regular,
S.atomic.forceFormula_all S.atomic_regular,S.atomic.forceFormula_imp S.atomic_regular,
ForcingQuotient.AtomicData.forceFormula_conj,ForcingQuotient.AtomicData.forceFormula_mem,
ForcingQuotient.AtomicData.forceFormula_ex,S.forces_edge]
have hv : v ∘ ![c,d,F] = ![v c,v d,v F] := by
ext i
fin_cases i <;> rfl
have hfun : S.atomic.ForceFormula ![v c,v d,v F] p (SetLanguage.functionOn 0 1) ↔
S.atomic.ForceFormula ![v c,v d] p (SetLanguage.functionOn 0 1) := by
simp only [SetLanguage.functionOn,S.atomic.forceFormula_rename S.atomic_regular]
have hc : ![v c,v d,v F] ∘ ![0,1] = ![v c,v d] ∘ ![0,1] := by
ext i
fin_cases i <;> rfl
rw [hc]
simpa [hv,Fin.snoc,Fin.castPred,Fin.castLT] using
and_congr hfun (Iff.rfl :
(∀ x y : S.Name, ∀ q, q ≤ p → S.atomic.MemF q x (v d) →
∀ r, r ≤ q → S.App r (v F) x y →
∀ s, s ≤ r → ∃ t, t ≤ s ∧ ∃ z : S.Name,
S.App t (v c) x z ∧ S.atomic.MemF t z y) ↔ _)
theorem forces_familyMember (F x z : S.Name) (p : P) :
S.Forces ![F,x,z] p SetLanguage.familyMember ↔
∀ q, q ≤ p → ∃ r, r ≤ q ∧ ∃ y : S.Name,
S.App r F x y ∧ S.atomic.MemF r z y := by
simp only [Forces,SetLanguage.familyMember,ForcingQuotient.AtomicData.forceFormula_ex,
ForcingQuotient.AtomicData.forceFormula_conj,ForcingQuotient.AtomicData.forceFormula_mem,
S.forces_edge]
rfl
/-- A member of the domain of a forced nonempty family has a possible
choice value. Both the family's set value and the member are internal names. -/
theorem nonemptyFamily_member {n} (v : Fin n → S.Name) (p : P) (F d : Fin n)
(hf : S.Forces v p (SetLanguage.nonemptyFamily F d)) (x : S.Name)
(hx : S.atomic.MemF p x (v d)) :
S.Forces ![v F,x] p SetLanguage.familyMember.ex := by
obtain ⟨hfun,hne⟩ := (S.forces_nonemptyFamily v p F d).mp hf
intro q hqp
obtain ⟨r,hrq,y,ha,_⟩ := S.functionOn_total ![v F,v d] p 0 1 hfun x le_rfl hx q hqp
obtain ⟨s,hsr,z,hz⟩ := hne x y p le_rfl hx r (hrq.trans hqp) ha r le_rfl
refine ⟨s,hsr.trans hrq,z,?_⟩
have hvec : Fin.snoc ![v F,x] z = ![v F,x,z] := by
ext i
fin_cases i <;> rfl
rw [hvec]
exact (S.forces_familyMember _ _ _ _).mpr (fun t hts =>
⟨t,le_rfl,y,S.app_mono (hts.trans hsr) ha,S.atomic.mem_mono hts hz⟩)
/-- Once the family's value at an index is specified, a selected member
belongs to that value. This uses single-valuedness of the actual graph. -/
theorem familyMember_mem {n} (v : Fin n → S.Name) (p : P) (F d : Fin n)
(hfun : S.Forces v p (SetLanguage.functionOn F d)) (x y z : S.Name)
(hx : S.atomic.MemF p x (v d)) (ha : S.App p (v F) x y)
(hz : S.Forces ![v F,x,z] p SetLanguage.familyMember) : S.atomic.MemF p z y := by
apply S.atomic_regular.2
intro q hqp
obtain ⟨r,hrq,t,hat,hzt⟩ := (S.forces_familyMember _ _ _ _).mp hz q hqp
have he := S.functionOn_unique v r F d (S.atomic.forceFormula_mono (hrq.trans hqp) hfun)
x t y (S.atomic.mem_mono (hrq.trans hqp) hx) hat (S.app_mono (hrq.trans hqp) ha)
exact ⟨r,hrq,(S.atomic.mem_congr (S.atomic.eq_refl r z) he).mp hzt⟩
/-- The ordinary first-order ACwo sentence follows from dense internal
choice graphs. This is only a logical unpacking, with the ordinal and all
family hypotheses unchanged. -/
theorem forces_ACwo_of_dense
(h : ∀ (p : P) (η F : S.Name),
S.Forces ![η] p (SetLanguage.ordinal 0) →
S.Forces ![F,η] p (SetLanguage.nonemptyFamily 0 1) →
∃ q, q ≤ p ∧ ∃ c : S.Name,
S.Forces ![c,η,F] q (SetLanguage.choiceForFamily 0 1 2)) (p : P) :
S.Forces Fin.elim0 p SetLanguage.ACwo := by
change S.atomic.ForceFormula Fin.elim0 p SetLanguage.ACwo
rw [SetLanguage.ACwo,S.atomic.forceFormula_all S.atomic_regular]
intro η
have hη : Fin.snoc (Fin.elim0 : Fin 0 → S.Name) η = ![η] := by
ext i
fin_cases i
rfl
rw [hη]
rw [S.atomic.forceFormula_imp S.atomic_regular]
intro q hqp ho
rw [S.atomic.forceFormula_all S.atomic_regular]
intro F
have hF : Fin.snoc ![η] F = ![η,F] := by
ext i
fin_cases i <;> rfl
rw [hF]
rw [S.atomic.forceFormula_imp S.atomic_regular]
intro r hrq hf
have hf' : S.Forces ![F,η] r (SetLanguage.nonemptyFamily 0 1) :=
(S.forces_nonemptyFamily ![F,η] r 0 1).mpr
((S.forces_nonemptyFamily ![η,F] r 1 0).mp hf)
intro s hsr
obtain ⟨t,hts,c,hc⟩ := h s η F (S.atomic.forceFormula_mono (hsr.trans hrq) ho)
(S.atomic.forceFormula_mono hsr hf')
refine ⟨t,hts,c,?_⟩
have hcvec : Fin.snoc ![η,F] c = ![η,F,c] := by
ext i
fin_cases i <;> rfl
rw [hcvec]
exact (S.forces_choiceForFamily ![η,F,c] t 2 0 1).mpr
((S.forces_choiceForFamily ![c,η,F] t 0 1 2).mp hc)
end
end PartitionConsistency.SetForcingNames.SymmetricSystem
namespace PartitionConsistency.SetForcingNames.SymmetricSystem
universe u v w
noncomputable section
variable {P : Type w} [PartialOrder P] [OrderTop P] {Γ : Type v} [Group Γ]
variable (S : SymmetricSystem.{u} P Γ)
/-- Uniformly supported local choices yield an actual internal set function,
not an external function substituted for the conclusion of ACwo. -/
theorem indexedGraph_choiceForFamily (X : ZFSet.{u}) (F : S.Name)
(f : X → S.Name) (H : Subgroup Γ) (hH : H ∈ S.filter)
(hfix : ∀ g ∈ H, ∀ i, g • f i = f i) (p : P)
(hfun : S.Forces ![F,Name.check X] p (SetLanguage.functionOn 0 1))
(hf : ∀ i : X, S.Forces ![F,Name.check i.val,f i] p SetLanguage.familyMember) :
S.Forces ![S.indexedGraph X f H hH hfix,Name.check X,F] p
(SetLanguage.choiceForFamily 0 1 2) := by
apply (S.forces_choiceForFamily _ _ _ _ _).mpr
refine ⟨S.indexedGraph_functionOn X f H hH hfix p,?_⟩
intro x y q hqp hx r hrq ha s hsr
obtain ⟨t,hts,i,hi,heq⟩ := (S.mem_check X x q).mp hx s (hsr.trans hrq)
let j : X := ⟨i,hi⟩
have hap : S.App t F (Name.check i) y :=
(S.app_congr (S.atomic.eq_refl t F) heq (S.atomic.eq_refl t y)).mp
(S.app_mono (hts.trans hsr) ha)
have hm := S.familyMember_mem ![F,Name.check X] t 0 1
(S.atomic.forceFormula_mono (hts.trans (hsr.trans (hrq.trans hqp))) hfun)
(Name.check i) y (f j) (S.check_mem_of_mem hi t) hap
(S.atomic.forceFormula_mono (hts.trans (hsr.trans (hrq.trans hqp))) (hf j))
refine ⟨t,hts,f j,?_,hm⟩
exact (S.app_congr (S.atomic.eq_refl t _) heq (S.atomic.eq_refl t _)).mpr
(S.indexedGraph_app_at X f H hH hfix j t)
end
end PartitionConsistency.SetForcingNames.SymmetricSystem
/-! ## ACwo -/
namespace PartitionConsistency.ProductForcing
universe u
open SetForcingNames SetForcingNames.SymmetricSystem DiagramForcing
noncomputable section
variable {M I κ K : Type u} [LeftCancelMonoid M] [DiagramOrder.IsConical M]
variable {μ : Cardinal.{u}} (hμ : Cardinal.aleph0 ≤ μ)
/-- One previously chosen extension of the supporting diagram supports all
choices from a ground-indexed family, at arbitrary name ranks. The result is
an internal graph; the uniform maximum principle only constructs its name. -/
theorem ground_family_choice [Infinite M] [Infinite I] [Uncountable K]
(hcard : Cardinal.mk M = μ) (hsize : Cardinal.mk M < Cardinal.mk I)
(hmerger : HasFiniteMergers M) (e : M)
(he : Cardinal.mk ((Set.range (fun x : M => e * x))ᶜ : Set M) = Cardinal.mk M)
(hprobes : RootProbes e K) (X : ZFSet.{u})
(F : (system (M := M) (I := I) (κ := κ) hμ).Name)
(p q : Diagram M I) (hq : q.sub e = p)
(hF : ∀ π ∈ SupportFilter.Fix p.range, π • F = F)
(d₀ : CohenForcing.Condition I κ) (hd₀ : d₀.support ⊆ q.range)
(hf : (system hμ).Forces ![F,Name.check X] ((d₀,p) : Poset M I κ)
(SetLanguage.nonemptyFamily 0 1)) :
∃ c : (system (M := M) (I := I) (κ := κ) hμ).Name,
(system hμ).Forces ![c,Name.check X,F] ((d₀,q) : Poset M I κ)
(SetLanguage.choiceForFamily 0 1 2) := by
let S := system (M := M) (I := I) (κ := κ) hμ
have hw (i : X) : ∃ ν : S.Name,
(∀ π ∈ SupportFilter.Fix q.range, π • ν = ν) ∧
S.Forces ![F,Name.check i.val,ν] ((d₀,q) : Poset M I κ) SetLanguage.familyMember := by
have hv : ∀ π ∈ SupportFilter.Fix p.range, ∀ j : Fin 2,
π • (![F,Name.check i.val] : Fin 2 → S.Name) j = ![F,Name.check i.val] j := by
intro π hπ j
fin_cases j
· exact hF π hπ
· exact Name.smul_check S π _
have hm := S.nonemptyFamily_member ![F,Name.check X] ((d₀,p) : Poset M I κ) 0 1 hf
(Name.check i.val) (S.check_mem_of_mem i.property _)
obtain ⟨ν,hν,hforce⟩ := localized_maximum hμ hcard hsize hmerger e he hprobes
SetLanguage.familyMember ![F,Name.check i.val] p q hq hv d₀ hd₀ hm
refine ⟨ν,hν,?_⟩
have hvec : Fin.snoc ![F,Name.check i.val] ν = ![F,Name.check i.val,ν] := by
ext j
fin_cases j <;> rfl
rwa [hvec] at hforce
choose f hfix hforce using hw
let H := SupportFilter.Fix q.range
have hH : H ∈ S.filter := ⟨q.range,by rw [Diagram.cardinal_range,hcard],le_rfl⟩
have hf' := (S.forces_nonemptyFamily ![F,Name.check X] ((d₀,p) : Poset M I κ) 0 1).mp hf
exact ⟨S.indexedGraph X f H hH (fun π hπ i => hfix i π hπ),
S.indexedGraph_choiceForFamily X F f H hH (fun π hπ i => hfix i π hπ) _
(S.atomic.forceFormula_mono (p := ((d₀,p) : Poset M I κ)) (q := ((d₀,q) : Poset M I κ))
(WithTop.coe_le_coe.mpr ⟨le_rfl,⟨e,hq⟩⟩) hf'.1) hforce⟩
/-- An arbitrary starting condition for a ground-indexed nonempty family
can be strengthened to force a choice graph. The family's support and the
Cohen condition are both put in the root before using probes. -/
theorem ground_family_choice_dense [Infinite M] [Infinite I] [Uncountable K]
(hcard : Cardinal.mk M = μ) (hsize : Cardinal.mk M < Cardinal.mk I)
(hmerger : HasFiniteMergers M) (e : M)
(he : Cardinal.mk ((Set.range (fun x : M => e * x))ᶜ : Set M) = Cardinal.mk M)
(hprobes : RootProbes e K) (X : ZFSet.{u})
(F : (system (M := M) (I := I) (κ := κ) hμ).Name) (t : Poset M I κ)
(hf : (system hμ).Forces ![F,Name.check X] t (SetLanguage.nonemptyFamily 0 1)) :
∃ s, s ≤ t ∧ ∃ c : (system (M := M) (I := I) (κ := κ) hμ).Name,
(system hμ).Forces ![c,Name.check X,F] s (SetLanguage.choiceForFamily 0 1 2) := by
let S := system (M := M) (I := I) (κ := κ) hμ
obtain ⟨emb⟩ := (Cardinal.le_def M I).mp hsize.le
let : Nonempty (Diagram M I) := ⟨⟨emb⟩⟩
obtain ⟨d,hdt⟩ := exists_condition_below t
obtain ⟨J,hJ,hfix⟩ := name_support hμ F
have hU : Cardinal.mk ↥(J ∪ d.1.support) ≤ Cardinal.mk M := by
rw [hcard]
exact (Cardinal.mk_union_le _ _).trans
((add_le_add hJ (d.1.cardinal_support.trans hμ)).trans_eq (Cardinal.add_eq_self hμ))
obtain ⟨p,hp,hcover⟩ := Diagram.extend_through hsize e he d.2 hU
have hpd : ((d.1,p) : Poset M I κ) ≤ t :=
(WithTop.coe_le_coe.mpr (show (d.1,p) ≤ d from ⟨le_rfl,⟨e,hp⟩⟩)).trans hdt
obtain ⟨q,hq,_⟩ := Diagram.extend_through hsize e he p (J := ∅) (by simp)
have hqp : q ≤ p := ⟨e,hq⟩
obtain ⟨c,hc⟩ := ground_family_choice hμ hcard hsize hmerger e he hprobes X F p q hq
(fun π hπ => hfix π ((SupportFilter.mem_Fix _ _).mpr
(fun j hj => (SupportFilter.mem_Fix _ _).mp hπ j (hcover (Or.inl hj)))))
d.1 (fun j hj => Diagram.range_antitone hqp (hcover (Or.inr hj)))
(S.atomic.forceFormula_mono hpd hf)
exact ⟨(d.1,q),(WithTop.coe_le_coe.mpr (show (d.1,q) ≤ (d.1,p) from ⟨le_rfl,hqp⟩)).trans hpd,c,hc⟩
/-- Choice for every internal ordinal-indexed family, without a rank cutoff.
Ordinal preservation first decides the index set to a ground ordinal, after
which one uniformly supported internal choice graph is constructed. -/
theorem forces_ACwo [Infinite M] [Infinite I] [Uncountable K]
(hcard : Cardinal.mk M = μ) (hsize : Cardinal.mk M < Cardinal.mk I)
(hmerger : HasFiniteMergers M) (e : M)
(he : Cardinal.mk ((Set.range (fun x : M => e * x))ᶜ : Set M) = Cardinal.mk M)
(hprobes : RootProbes e K) (p : Poset M I κ) :
(system (M := M) (I := I) (κ := κ) hμ).Forces Fin.elim0 p SetLanguage.ACwo := by
let S := system (M := M) (I := I) (κ := κ) hμ
apply S.forces_ACwo_of_dense
intro s η F ho hf'
obtain ⟨t,hts,β,hη⟩ := S.forces_ordinal_decide ![η] s 0 ho s le_rfl
have hf' := S.atomic.forceFormula_mono hts hf'
have hchange : S.Forces ![F,Name.check β.toZFSet] t (SetLanguage.nonemptyFamily 0 1) := by
apply (S.atomic.forceFormula_tuple_congr (p := t) (φ := SetLanguage.nonemptyFamily 0 1)
(v := ![F,η]) (w := ![F,Name.check β.toZFSet]) ?_).mp hf'
intro i
fin_cases i
· exact S.atomic.eq_refl t F
· exact hη
obtain ⟨a,hat,c,hc⟩ := ground_family_choice_dense hμ hcard hsize hmerger e he hprobes
β.toZFSet F t hchange
have hc' : S.Forces ![c,η,F] a (SetLanguage.choiceForFamily 0 1 2) := by
apply (S.atomic.forceFormula_tuple_congr (p := a) (φ := SetLanguage.choiceForFamily 0 1 2)
(v := ![c,Name.check β.toZFSet,F]) (w := ![c,η,F]) ?_).mp hc
intro i
fin_cases i
· exact S.atomic.eq_refl a c
· exact S.atomic.eq_symm (S.atomic.eq_mono hat hη)
· exact S.atomic.eq_refl a F
exact ⟨a,hat.trans hts,c,hc'⟩
end
end PartitionConsistency.ProductForcing
namespace PartitionConsistency.ConcreteSystem
open MonoidConstruction CardinalParameters DiagramForcing SetForcingNames
noncomputable section
instance : Uncountable K := Cardinal.aleph0_lt_mk_iff.mp
(by rw [cardinal_K]; exact Cardinal.aleph0_lt_aleph_one.trans_le aleph_one_le_μ)
/-- The probes used by ordinal choice are actually present in the saturated
monoid. This is an instance of the executed requests with `a=1`. -/
theorem rootProbes : ProductForcing.RootProbes T.e K := by
intro b hb
let d : ProbeData T :=
⟨1,b,hb,⟨fun _ => 1,rfl,fun _ => dvd_refl _,fun _ => dvd_refl _⟩⟩
obtain ⟨m,_,hm,hi⟩ := Saturation.probes Base.object K d
refine ⟨m,fun i => (hm i).exit.trans (one_mul _),?_⟩
intro i j hij z
have hh := hi i j hij z
change m i ∣ z ∧ m j ∣ z ↔ (1 : T) * T.e ∣ z at hh
simpa only [one_mul] using! hh
/-- No additional cardinal or support principle is assumed here. -/
theorem forces_ACwo (p : P) : S.Forces Fin.elim0 p SetLanguage.ACwo :=
ProductForcing.forces_ACwo aleph0_le_μ cardinal_T size_lt finiteMergers T.e
complement_cardinal rootProbes p
/-- Consistency of the ZF + ACwo + ¬AC subtheory. The full target with
PP is proved below in `consistent_target`. -/
theorem consistent_ZF_ACwo_not_AC :
Consistent (SetLanguage.ZF ∪ {SetLanguage.ACwo,SetLanguage.AC.neg}) := by
apply S.consistent_of_forces (⊤ : P)
intro φ hφ
rcases hφ with hφ | hφ
· exact forces_ZF ⊤ φ hφ
· rcases hφ with rfl | rfl | hfalse
· exact forces_ACwo ⊤
· exact forces_not_AC ⊤
end
end PartitionConsistency.ConcreteSystem
end OAI