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import OAI.Dynamics.SmoothObstruction.InvariantMeasure
import OAI.Dynamics.SmoothObstruction.StandardProbability
namespace OAI
section
open MeasureTheory Set Filter Topology
namespace SmoothObstruction.PhaseDynamics
variable {X : Type*} [MeasurableSpace X] [MeasurableSingletonClass X]
omit [MeasurableSpace X] [MeasurableSingletonClass X] in
lemma iterate_phase {m : ℕ} (T : X → X) (a : X → ZMod m)
(ha : ∀ x, a (T x) = a x + 1) (x : X) (n : ℕ) :
a ((T^[n]) x) = a x + n := by
induction n with
| zero => simp
| succ n ih =>
rw [Function.iterate_succ_apply', ha, ih, Nat.cast_add, Nat.cast_one, add_assoc]
omit [MeasurableSpace X] [MeasurableSingletonClass X] in
/-- Uniform infinite cyclic factors rule out every periodic point. This
uses only the exact phase evolution, not recognition or word frequencies. -/
theorem no_periodic_points (T : X → X) (m : ℕ → ℕ) (a : ∀ i, X → ZMod (m i))
(ha : ∀ i x, a i (T x) = a i x + 1) (hm : ∀ n, ∃ i, n < m i) :
∀ x n, 0 < n → (T^[n]) x ≠ x := by
intro x n hn hx
obtain ⟨i, hi⟩ := hm n
have h := iterate_phase T (a i) (ha i) x n
rw [hx] at h
have hn0 : (n : ZMod (m i)) = 0 := by
apply add_left_cancel (a := a i x)
simpa using h.symm
have hdiv := (ZMod.natCast_eq_zero_iff n (m i)).mp hn0
exact (not_le.mpr hi) (Nat.le_of_dvd hn hdiv)
/-- The phase extension's nonatomicity: a positive singleton would return by
Poincare recurrence, contradicting its arbitrarily large cyclic factors. -/
theorem noAtoms_of_phases (μ : Measure X) [IsFiniteMeasure μ] (T : X → X)
(hT : MeasurePreserving T μ μ) (m : ℕ → ℕ) (a : ∀ i, X → ZMod (m i))
(ha : ∀ i x, a i (T x) = a i x + 1) (hm : ∀ n, ∃ i, n < m i) : NullSingletonClass μ := by
refine ⟨fun x => ?_⟩
by_contra hx
obtain ⟨y, hy, n, hn, hny⟩ := hT.conservative.exists_mem_iterate_mem'
(measurableSet_singleton x) hx
have hyx : y = x := mem_singleton_iff.mp hy
subst y
exact no_periodic_points T m a ha hm x n (Nat.pos_of_ne_zero hn) (mem_singleton_iff.mp hny)
section Ambient
variable (A : Type*) [TopologicalSpace A] (m : ℕ → ℕ)
abbrev Space := (ℤ → A) × ∀ i, ZMod (m i)
/-- The source map: bilateral symbol shift and addition of one in every
phase. Its inverse subtracts one, with no modulo-null restriction. -/
def shift : Space A m ≃ₜ Space A m where
toFun x := (fun t => x.1 (t + 1), fun i => x.2 i + 1)
invFun x := (fun t => x.1 (t - 1), fun i => x.2 i - 1)
left_inv x := by ext <;> simp
right_inv x := by ext <;> simp
continuous_toFun := by
apply Continuous.prodMk
· exact continuous_pi (fun t => (continuous_apply (t + 1)).comp continuous_fst)
· exact continuous_pi (fun i => ((continuous_apply i).comp continuous_snd).add continuous_const)
continuous_invFun := by
apply Continuous.prodMk
· exact continuous_pi (fun t => (continuous_apply (t - 1)).comp continuous_fst)
· exact continuous_pi (fun i => ((continuous_apply i).comp continuous_snd).sub continuous_const)
@[simp] lemma shift_symbol (x : Space A m) (t : ℤ) : (shift A m x).1 t = x.1 (t + 1) := rfl
@[simp] lemma shift_phase (x : Space A m) (i : ℕ) : (shift A m x).2 i = x.2 i + 1 := rfl
end Ambient
section Words
variable {A : Type*} [TopologicalSpace A] [DiscreteTopology A]
(m : ℕ → ℕ) (hm : ∀ i, m i ∣ m (i + 1))
(W : ∀ i, Set (Fin (m i) → A))
/-- Level-i symbols beginning at an integer time. -/
def wordAt (x : Space A m) (i : ℕ) (t : ℤ) : Fin (m i) → A :=
fun j => x.1 (t + j.val)
/-- Exact compatibility of phases through the canonical cyclic quotient. -/
def Compatible (x : Space A m) (i : ℕ) : Prop :=
ZMod.castHom (hm i) (ZMod (m i)) (x.2 (i + 1)) = x.2 i
/-- Every level boundary carries a legal word; the sign convention records
the index of the origin inside its word, exactly as in source section 6. -/
def Legal (x : Space A m) (i : ℕ) : Prop :=
∀ t : ℤ, (t : ZMod (m i)) = -x.2 i → wordAt m x i t ∈ W i
def extension : Set (Space A m) :=
{x | ∀ i, Compatible m hm x i ∧ Legal m W x i}
omit [DiscreteTopology A] in
lemma continuous_wordAt (i : ℕ) (t : ℤ) : Continuous (fun x : Space A m => wordAt m x i t) :=
continuous_pi (fun j => (continuous_apply (t + j.val)).comp continuous_fst)
omit [DiscreteTopology A] in
lemma compatible_closed (i : ℕ) : IsClosed {x : Space A m | Compatible m hm x i} := by
apply isClosed_eq _ ((continuous_apply i).comp continuous_snd)
exact (continuous_of_discreteTopology : Continuous (ZMod.castHom (hm i) (ZMod (m i)))).comp
((continuous_apply (i + 1)).comp continuous_snd)
lemma legal_closed (i : ℕ) : IsClosed {x : Space A m | Legal m W x i} := by
have heq : {x : Space A m | Legal m W x i} =
⋂ t : ℤ, ({x : Space A m | (t : ZMod (m i)) ≠ -x.2 i} ∪
(fun x : Space A m => wordAt m x i t) ⁻¹' W i) := by
ext x
simp only [mem_ofPred_eq, mem_iInter, mem_union, mem_preimage, Legal]
simp only [imp_iff_not_or]
rw [heq]
apply isClosed_iInter
intro t
apply IsClosed.union _ ((isClosed_discrete (W i)).preimage (continuous_wordAt m i t))
have hc : IsClosed {a : ZMod (m i) | (t : ZMod (m i)) ≠ -a} := isClosed_discrete _
exact hc.preimage (show Continuous (fun x : Space A m => x.2 i) from
(continuous_apply i).comp continuous_snd)
lemma extension_closed : IsClosed (extension m hm W) := by
have heq : extension m hm W =
⋂ i, {x : Space A m | Compatible m hm x i} ∩ {x : Space A m | Legal m W x i} := by
ext x; simp [extension]
rw [heq]
exact isClosed_iInter (fun i => (compatible_closed m hm i).inter (legal_closed m W i))
omit [DiscreteTopology A] in
lemma compatible_shift_iff (x : Space A m) (i : ℕ) :
Compatible m hm (shift A m x) i ↔ Compatible m hm x i := by
simp [Compatible, shift, map_add, map_one]
omit [DiscreteTopology A] in
lemma legal_shift_iff (x : Space A m) (i : ℕ) :
Legal m W (shift A m x) i ↔ Legal m W x i := by
constructor
· intro h t ht
have hb : ((t - 1 : ℤ) : ZMod (m i)) = -(shift A m x).2 i := by
simp only [Int.cast_sub, Int.cast_one, shift_phase]
rw [ht]
ring
have hw := h (t - 1) hb
convert hw using 1
ext j
change x.1 (t + (j.val : ℤ)) = x.1 (t - 1 + (j.val : ℤ) + 1)
exact congrArg x.1 (by ring)
· intro h t ht
have hb : ((t + 1 : ℤ) : ZMod (m i)) = -x.2 i := by
simp only [Int.cast_add, Int.cast_one]
rw [ht, shift_phase]
ring
have hw := h (t + 1) hb
convert hw using 1
ext j
change x.1 (t + (j.val : ℤ) + 1) = x.1 (t + 1 + (j.val : ℤ))
exact congrArg x.1 (by ring)
omit [DiscreteTopology A] in
lemma extension_shift_iff (x : Space A m) :
shift A m x ∈ extension m hm W ↔ x ∈ extension m hm W := by
simp only [extension, mem_ofPred_eq, compatible_shift_iff, legal_shift_iff]
omit [DiscreteTopology A] in
lemma extension_shift_symm (x : Space A m) (hx : x ∈ extension m hm W) :
(shift A m).symm x ∈ extension m hm W := by
apply (extension_shift_iff m hm W ((shift A m).symm x)).mp
simpa using hx
/-- Restriction to the genuine closed phase extension, in both directions. -/
def extensionShift : extension m hm W ≃ₜ extension m hm W where
toFun x := ⟨shift A m x.val, (extension_shift_iff m hm W x.val).mpr x.property⟩
invFun x := ⟨(shift A m).symm x.val, extension_shift_symm m hm W x.val x.property⟩
left_inv x := Subtype.ext ((shift A m).left_inv x.val)
right_inv x := Subtype.ext ((shift A m).right_inv x.val)
continuous_toFun := ((shift A m).continuous.comp continuous_subtype_val).subtype_mk _
continuous_invFun := ((shift A m).symm.continuous.comp continuous_subtype_val).subtype_mk _
/-- Compactness needs only finite-level admissible configurations. The actual
word hierarchy supplies these by periodically repeating a word at the largest
requested level; no invariant measure or frequency hypothesis enters. -/
theorem extension_nonempty [CompactSpace A] [∀ i, NeZero (m i)]
(hfinite : ∀ n, ∃ x : Space A m, ∀ i ≤ n, Compatible m hm x i ∧ Legal m W x i) :
(extension m hm W).Nonempty := by
let E : ℕ → Set (Space A m) := fun n =>
{x | ∀ i ≤ n, Compatible m hm x i ∧ Legal m W x i}
have hcl (n : ℕ) : IsClosed (E n) := by
have heq : E n = ⋂ i ∈ Set.Iic n,
{x : Space A m | Compatible m hm x i} ∩ {x : Space A m | Legal m W x i} := by
ext x; simp [E]
rw [heq]
exact isClosed_biInter (fun i _ => (compatible_closed m hm i).inter (legal_closed m W i))
obtain ⟨x, hx⟩ := IsCompact.nonempty_iInter_of_sequence_nonempty_isCompact_isClosed E
(fun n x hx i hi => hx i (by omega)) hfinite (hcl 0).isCompact hcl
refine ⟨x, fun i => ?_⟩
exact (mem_iInter.mp hx i) i le_rfl
end Words
end SmoothObstruction.PhaseDynamics
end
section
namespace SmoothObstruction.PhaseDynamics
open MeasureTheory Set Filter
open scoped Topology
variable {A : Type} [Fintype A] [Nonempty A] [TopologicalSpace A]
[DiscreteTopology A] [MeasurableSpace A] [BorelSpace A]
(m : ℕ → ℕ) [∀ i, NeZero (m i)] (hm : ∀ i, m i ∣ m (i+1))
(W : ∀ i, Set (Fin (m i) → A))
omit [Fintype A] [Nonempty A] [TopologicalSpace A] [DiscreteTopology A] [BorelSpace A]
[∀ i, NeZero (m i)] in
lemma extension_coordinate_space :
(inferInstance : MeasurableSpace (extension m hm W)) = MeasurableSpace.comap
(PhaseEntropy.coordinates (fun x : extension m hm W => x.val.1)
(fun x : extension m hm W => x.val.2)) MeasurableSpace.pi := by
let e := MeasurableEquiv.sumPiEquivProdPi (PhaseEntropy.Coordinate A m)
have he := e.symm.measurableEmbedding.comap_eq
have hc : PhaseEntropy.coordinates (fun x : extension m hm W => x.val.1)
(fun x : extension m hm W => x.val.2) = e.symm ∘ Subtype.val := by
funext x i
cases i <;> rfl
change MeasurableSpace.comap (Subtype.val : extension m hm W → Space A m)
inferInstance = _
exact (congrArg (MeasurableSpace.comap (Subtype.val : extension m hm W → Space A m)) he).symm.trans
(MeasurableSpace.comap_comp.trans (congrArg (fun f => MeasurableSpace.comap f MeasurableSpace.pi) hc.symm))
/-- A genuine ergodic invertible standard nonatomic finite-KS system from
any nonempty finite admissible word hierarchy with unbounded lengths.
This is the measure-theoretic construction, not its graph obstruction. -/
theorem exists_system
(hunbounded : ∀ n, ∃ i, n < m i)
(hfinite : ∀ n, ∃ x : Space A m, ∀ i ≤ n, Compatible m hm x i ∧ Legal m W x i) :
∃ μ : ProbabilityMeasure (extension m hm W),
StandardNonatomic (μ : Measure (extension m hm W)) ∧
Ergodic (extensionShift m hm W) (μ : Measure (extension m hm W)) ∧
FiniteKSEntropy (μ : Measure (extension m hm W)) (extensionShift m hm W) := by
let : CompactSpace A := Finite.compactSpace
let : Fact (IsClosed (extension m hm W)) := ⟨extension_closed m hm W⟩
let : CompactSpace (extension m hm W) := isCompact_iff_compactSpace.mp (extension_closed m hm W).isCompact
have hn := extension_nonempty m hm W hfinite
let : Nonempty (extension m hm W) := hn.to_subtype
let : StandardBorelSpace (extension m hm W) := (extension_closed m hm W).measurableSet.standardBorel
obtain ⟨μ,hμ⟩ := CompactInvariant.exists_ergodic_probability
(extensionShift m hm W) (extensionShift m hm W).continuous
let : NullSingletonClass (μ : Measure (extension m hm W)) :=
noAtoms_of_phases μ (extensionShift m hm W) hμ.toMeasurePreserving m
(fun i x => x.val.2 i) (fun _ _ => rfl) hunbounded
refine ⟨μ,standardNonatomic_of_standardBorel (μ : Measure (extension m hm W)),hμ,?_⟩
exact PhaseEntropy.finiteKS (fun x : extension m hm W => x.val.1)
(fun x : extension m hm W => x.val.2) μ hμ.toMeasurePreserving
(extension_coordinate_space m hm W) (fun _ _ => rfl) (fun _ _ => rfl)
end SmoothObstruction.PhaseDynamics
end
end OAI
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