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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
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