import Mathlib namespace OAI open scoped BigOperators ENNReal NNReal Topology ContDiff open MeasureTheory namespace AlternatingNS theorem neZeroThree : NeZero 3 := ⟨Nat.succ_ne_zero 2⟩ theorem twoAtLeastTwo : Nat.AtLeastTwo 2 := ⟨Nat.le_refl 2⟩ theorem threeAtLeastTwo : Nat.AtLeastTwo 3 := ⟨Nat.le_succ 2⟩ theorem eightAtLeastTwo : Nat.AtLeastTwo 8 := ⟨by decide⟩ abbrev Rule := ℕ × ℕ × Fin 3 abbrev Machine := ℕ × ℕ × ℕ × List ℕ × List (Option Rule) namespace Machine def states (M : Machine) : ℕ := M.1 + 1 def alphabet (M : Machine) : ℕ := M.2.1 + 1 def initialState (M : Machine) : ℕ := M.2.2.1 def haltingStates (M : Machine) : List ℕ := M.2.2.2.1 def table (M : Machine) : List (Option Rule) := M.2.2.2.2 def instruction (M : Machine) (q a : ℕ) : Option Rule := (M.table[q * M.alphabet + a]?).join def WellFormed (M : Machine) : Prop := M.initialState < M.states ∧ (∀ q ∈ M.haltingStates, q < M.states) ∧ ∀ q a r, q < M.states → a < M.alphabet → M.instruction q a = some r → r.1 < M.states ∧ r.2.1 < M.alphabet def ValidInput (M : Machine) (w : List ℕ) : Prop := ∀ a ∈ w, a < M.alphabet structure Configuration where state : ℕ head : ℤ tape : ℤ → ℕ def isHalting (M : Machine) (c : Configuration) : Bool := decide (c.state = M.states ∨ c.state ∈ M.haltingStates) def initial (M : Machine) (w : List ℕ) : Configuration where state := M.initialState head := 0 tape := fun i => if 0 ≤ i then w[i.toNat]?.getD 0 else 0 def step (M : Machine) (c : Configuration) : Configuration := if M.isHalting c then c else match M.instruction c.state (c.tape c.head) with | none => { c with state := M.states } | some r => { state := r.1 head := c.head + ((r.2.2.val : ℤ) - 1) tape := Function.update c.tape c.head r.2.1 } def run (M : Machine) (w : List ℕ) (n : ℕ) : Configuration := (M.step)^[n] (M.initial w) def Halts (M : Machine) (w : List ℕ) : Prop := ∃ n : ℕ, M.isHalting (M.run w n) = true end Machine abbrev Space := EuclideanSpace ℝ (Fin 3) abbrev Field (E : Type*) := ℝ → Space → E abbrev Velocity := Field Space abbrev Pressure := Field ℝ abbrev MultiIndex := Fin 3 → ℕ noncomputable section def e (i : Fin 3) : Space := EuclideanSpace.single i 1 def dx {E : Type*} [NormedAddCommGroup E] [NormedSpace ℝ E] (i : Fin 3) (F : Field E) : Field E := fun t x => fderiv ℝ (F t) x (e i) def dt {E : Type*} [NormedAddCommGroup E] [NormedSpace ℝ E] (F : Field E) : Field E := fun t x => fderivWithin ℝ (fun s => F s x) (Set.Ici 0) t 1 def spatial {E : Type*} [NormedAddCommGroup E] [NormedSpace ℝ E] (α : MultiIndex) (F : Field E) : Field E := (dx 0)^[α 0] ((dx 1)^[α 1] ((dx 2)^[α 2] F)) def mixed {E : Type*} [NormedAddCommGroup E] [NormedSpace ℝ E] (l : ℕ) (α : MultiIndex) (F : Field E) : Field E := dt^[l] (spatial α F) def div (u : Velocity) (t : ℝ) (x : Space) : ℝ := ∑ i : Fin 3, dx i u t x i def grad (p : Pressure) (t : ℝ) (x : Space) : Space := (EuclideanSpace.equiv (Fin 3) ℝ).symm (fun i => dx i p t x) def laplacian (u : Velocity) (t : ℝ) (x : Space) : Space := ∑ i : Fin 3, dx i (dx i u) t x def advection (u : Velocity) (t : ℝ) (x : Space) : Space := fderiv ℝ (u t) x (u t x) def residual (ν : ℝ) (u : Velocity) : Velocity := fun t x => dt u t x + advection u t x - ν • laplacian u t x def timeCylinder (T : ℝ) : Set (ℝ × Space) := Set.Icc 0 T ×ˢ Set.univ def Smooth {E : Type*} [NormedAddCommGroup E] [NormedSpace ℝ E] (F : Field E) : Prop := ContDiffOn ℝ (∞) (Function.uncurry F) (Set.Ici 0 ×ˢ Set.univ) def ClassicalRegularity (u : Velocity) (p : Pressure) : Prop := (∀ x, DifferentiableOn ℝ (fun t => u t x) (Set.Ici 0)) ∧ (∀ t, 0 ≤ t → Differentiable ℝ (u t)) ∧ (∀ t, 0 ≤ t → ∀ i, Differentiable ℝ (dx i u t)) ∧ (∀ t, 0 ≤ t → Differentiable ℝ (p t)) ∧ ∀ T, 0 ≤ T → ContinuousOn (Function.uncurry u) (timeCylinder T) ∧ ContinuousOn (Function.uncurry (dt u)) (timeCylinder T) ∧ (∀ i, ContinuousOn (Function.uncurry (dx i u)) (timeCylinder T)) ∧ (∀ i j, ContinuousOn (Function.uncurry (dx i (dx j u))) (timeCylinder T)) ∧ ContinuousOn (Function.uncurry p) (timeCylinder T) ∧ (∀ i, ContinuousOn (Function.uncurry (dx i p)) (timeCylinder T)) def ContinuousInH {E : Type*} [NormedAddCommGroup E] [NormedSpace ℝ E] (k : ℕ) (F : Field E) (T : ℝ) : Prop := ∀ α : MultiIndex, (∑ i, α i) ≤ k → ∃ g : ℝ → Lp E 2 (volume : Measure Space), ContinuousOn g (Set.Icc 0 T) ∧ ∀ t ∈ Set.Icc 0 T, ∀ᵐ x ∂(volume : Measure Space), (g t) x = spatial α F t x def C1InL2 (u : Velocity) (T : ℝ) : Prop := ∃ g g' : ℝ → Lp Space 2 (volume : Measure Space), ContinuousOn g (Set.Icc 0 T) ∧ ContinuousOn g' (Set.Icc 0 T) ∧ (∀ t ∈ Set.Icc 0 T, HasDerivWithinAt g (g' t) (Set.Icc 0 T) t) ∧ (∀ t ∈ Set.Icc 0 T, ∀ᵐ x ∂(volume : Measure Space), (g t) x = u t x) ∧ (∀ t ∈ Set.Icc 0 T, ∀ᵐ x ∂(volume : Measure Space), (g' t) x = dt u t x) def CompetitorEnergyClass (u : Velocity) (p : Pressure) : Prop := ∀ T, 0 ≤ T → ContinuousInH 2 u T ∧ C1InL2 u T ∧ ContinuousInH 1 p T ∧ ∃ C : ℝ, ∀ t ∈ Set.Icc 0 T, ∀ x, ‖u t x‖ ≤ C def EnergyClass (u : Velocity) (p : Pressure) : Prop := CompetitorEnergyClass u p ∧ ∀ T, 0 ≤ T → ∃ C : ℝ, ∀ t ∈ Set.Icc 0 T, ∀ x, ‖u t x‖ + ‖fderiv ℝ (u t) x‖ ≤ C def NavierStokes (ν : ℝ) (f u : Velocity) (p : Pressure) : Prop := ClassicalRegularity u p ∧ (∀ x, u 0 x = 0) ∧ ∀ t, 0 ≤ t → ∀ x, div u t x = 0 ∧ dt u t x + advection u t x = -grad p t x + ν • laplacian u t x + f t x def Rapid (F : Velocity) : Prop := ∀ J l : ℕ, ∀ α : MultiIndex, ∃ C : ℝ, 0 ≤ C ∧ ∀ t, 0 ≤ t → ∀ x, (1 + t + ‖x‖) ^ J * ‖mixed l α F t x‖ ≤ C def SupportedIn (F : Velocity) (K : Set Space) : Prop := ∀ t, 0 ≤ t → Function.support (F t) ⊆ K def IsTrajectory (u : Velocity) (a : Space) (γ : ℝ → Space) : Prop := γ 0 = a ∧ ∀ t, 0 ≤ t → HasDerivWithinAt γ (u t (γ t)) (Set.Ici 0) t def observedParticle : Space := (EuclideanSpace.equiv (Fin 3) ℝ).symm ![-1, 0, 0] abbrev RationalPoint := ℚ × ℚ × ℚ × ℚ abbrev RationalVector := ℚ × ℚ × ℚ abbrev IndexCode := ℕ × ℕ × ℕ abbrev Program := Nat.Partrec.Code abbrev FieldProgram := Program × Program × Program def Returns {A B : Type*} [Encodable A] [Encodable B] (c : Program) (a : A) (b : B) : Prop := Encodable.encode b ∈ c.eval (Encodable.encode a) def index (α : IndexCode) : MultiIndex := ![α.1, α.2.1, α.2.2] def rationalVector (q : RationalVector) : Space := (EuclideanSpace.equiv (Fin 3) ℝ).symm ![(q.1 : ℝ), (q.2.1 : ℝ), (q.2.2 : ℝ)] def rationalPoint (q : RationalPoint) : ℝ × Space := ((q.1 : ℝ), rationalVector q.2) def dyadicError (n : ℕ) : ℝ := (1 / 2 : ℝ) ^ n def ComputableReal (r : ℝ) : Prop := ∃ a : ℕ → ℚ, Computable (fun n => ((a n).num, (a n).den)) ∧ ∀ n, |r - (a n : ℝ)| ≤ dyadicError n def ProgramFor (c : FieldProgram) (F : Velocity) : Prop := (∀ (l : ℕ) (α : IndexCode) (q : RationalPoint) (k : ℕ), ∃ v : RationalVector, Returns c.1 (l, α, q, k) v ∧ (0 ≤ q.1 → ‖rationalVector v - mixed l (index α) F (rationalPoint q).1 (rationalPoint q).2‖ ≤ dyadicError k)) ∧ (∀ (l : ℕ) (α : IndexCode) (R k : ℕ), ∃ m : ℕ, Returns c.2.1 (l, α, R, k) m ∧ ∀ z z' : ℝ × Space, 0 ≤ z.1 → 0 ≤ z'.1 → ‖z‖ ≤ R → ‖z'‖ ≤ R → ‖z - z'‖ ≤ dyadicError m → ‖mixed l (index α) F z.1 z.2 - mixed l (index α) F z'.1 z'.2‖ ≤ dyadicError k) ∧ (∀ (J l : ℕ) (α : IndexCode), ∃ B : ℕ, Returns c.2.2 (J, l, α) B ∧ ∀ t, 0 ≤ t → ∀ x, (1 + t + ‖x‖) ^ J * ‖mixed l (index α) F t x‖ ≤ B) def AlternatingConclusion (ν : ℝ) : Prop := ∃ (compileForce compileVelocity : Machine × List ℕ → FieldProgram), Computable compileForce ∧ Computable compileVelocity ∧ ∃ K : Set Space, IsCompact K ∧ ∀ (M : Machine) (w : List ℕ), M.WellFormed → M.ValidInput w → ∃ (f U : Velocity) (X : Space → ℝ → Space), ProgramFor (compileForce (M, w)) f ∧ ProgramFor (compileVelocity (M, w)) U ∧ Smooth f ∧ Smooth U ∧ SupportedIn f K ∧ SupportedIn U K ∧ Rapid f ∧ Rapid U ∧ f = residual ν U ∧ NavierStokes ν f U (fun _ _ => 0) ∧ EnergyClass U (fun _ _ => 0) ∧ (∀ (v : Velocity) (p : Pressure), NavierStokes ν f v p → CompetitorEnergyClass v p → ∀ t, 0 ≤ t → ∀ x, v t x = U t x ∧ p t x = 0) ∧ (∀ a, IsTrajectory U a (X a)) ∧ (∀ a γ, IsTrajectory U a γ → ∀ t, 0 ≤ t → γ t = X a t) ∧ ((∃ t : ℝ, 0 ≤ t ∧ 0 < X observedParticle t 0) ↔ M.Halts w) end end AlternatingNS end OAI