import OAI.MathematicalPhysics.NavierStokes.ShearFlows.FieldExpressions namespace OAI /-! Coordinate changes in finite field expressions. This moves the planar processor's periodic phase from its third spatial coordinate to time. -/ namespace ForcedComputation open ShearFlows noncomputable def reindexPoint (σ : Fin 4 → Fin 4) (y : SpaceTime) : SpaceTime := (timeSpaceCoord (σ 0) y, fun j => timeSpaceCoord (σ j.succ) y) theorem timeSpaceCoord_reindex (σ : Fin 4 → Fin 4) (j : Fin 4) (y : SpaceTime) : timeSpaceCoord j (reindexPoint σ y) = timeSpaceCoord (σ j) y := by fin_cases j <;> rfl def _root_.OAI.ShearFlows.FieldExpr.reindex (σ : Fin 4 → Fin 4) : FieldExpr → FieldExpr | .const r => .const r | .atom j p => .atom (σ j) p | .add e f => .add (e.reindex σ) (f.reindex σ) | .mul e f => .mul (e.reindex σ) (f.reindex σ) theorem _root_.OAI.ShearFlows.FieldExpr.valid_reindex {e : FieldExpr} (he : e.Valid) (σ : Fin 4 → Fin 4) : (e.reindex σ).Valid := by induction e with | const => trivial | atom j p => exact he | add e f ih₁ ih₂ => exact ⟨ih₁ he.1, ih₂ he.2⟩ | mul e f ih₁ ih₂ => exact ⟨ih₁ he.1, ih₂ he.2⟩ theorem _root_.OAI.ShearFlows.FieldExpr.val_reindex (e : FieldExpr) (σ : Fin 4 → Fin 4) (y : SpaceTime) : (e.reindex σ).val y = e.val (reindexPoint σ y) := by induction e with | const => rfl | atom j p => simp only [FieldExpr.reindex, FieldExpr.val, timeSpaceCoord_reindex] | add e f ih₁ ih₂ => simp only [FieldExpr.reindex, FieldExpr.val, ih₁, ih₂] | mul e f ih₁ ih₂ => simp only [FieldExpr.reindex, FieldExpr.val, ih₁, ih₂] def timeHeightSwap : Fin 4 → Fin 4 := ![3, 1, 2, 0] theorem reindexPoint_timeHeightSwap (y : SpaceTime) : reindexPoint timeHeightSwap y = (y.2 2, atHeight (horizontal y.2) y.1) := by apply Prod.ext · rfl · ext j fin_cases j <;> rfl theorem _root_.OAI.ShearFlows.FieldExpr.val_timeHeightSwap (e : FieldExpr) (y : SpaceTime) : (e.reindex timeHeightSwap).val y = e.val (y.2 2, atHeight (horizontal y.2) y.1) := by rw [FieldExpr.val_reindex, reindexPoint_timeHeightSwap] end ForcedComputation end OAI