import Mathlib import OAI.MathematicalPhysics.SheetFlows.ScheduledForce import OAI.MathematicalPhysics.SheetFlows.JetProfiles namespace OAI /-! SheetFlows box jets. -/ noncomputable section open Set MeasureTheory Filter open scoped BigOperators Topology namespace Solenoidal def coordinateLinear : Fin 4 → SpaceTime →L[ℝ] ℝ := ![ContinuousLinearMap.fst ℝ ℝ Space, (ContinuousLinearMap.proj 0).comp (ContinuousLinearMap.snd ℝ ℝ Space), (ContinuousLinearMap.proj 1).comp (ContinuousLinearMap.snd ℝ ℝ Space), (ContinuousLinearMap.proj 2).comp (ContinuousLinearMap.snd ℝ ℝ Space)] @[simp] theorem coordinateLinear_eq (j : Fin 4) (z : SpaceTime) : coordinateLinear j z = flatten z j := by fin_cases j <;> rfl @[simp] theorem coordinateLinear_basis (i j : Fin 4) : coordinateLinear i (spacetimeBasis j) = if i=j then 1 else 0 := by fin_cases i <;> fin_cases j <;> simp [coordinateLinear, spacetimeBasis, basis] inductive BoxExpr where | const : ℚ → BoxExpr | coord : Fin 4 → JetExpr → BoxExpr | add : BoxExpr → BoxExpr → BoxExpr | mul : BoxExpr → BoxExpr → BoxExpr namespace BoxExpr def eval : BoxExpr → SpaceTime → ℝ | .const q => fun _ => q | .coord j e => fun z => e.eval (coordinateLinear j z) | .add e f => fun z => e.eval z + f.eval z | .mul e f => fun z => e.eval z * f.eval z theorem smooth (e : BoxExpr) : ContDiff ℝ (⊤ : ℕ∞) e.eval := by induction e with | const q => exact contDiff_const | coord j e => exact e.smooth.comp (coordinateLinear j).contDiff | add e f he hf => exact he.add hf | mul e f he hf => exact he.mul hf def diff (j : Fin 4) : BoxExpr → BoxExpr | .const _ => .const 0 | .coord i e => if i=j then .coord i e.diff else .const 0 | .add e f => .add (e.diff j) (f.diff j) | .mul e f => .add (.mul (e.diff j) f) (.mul e (f.diff j)) theorem diff_correct (e : BoxExpr) (j : Fin 4) (z : SpaceTime) : (e.diff j).eval z = fderiv ℝ e.eval z (spacetimeBasis j) := by induction e with | const q => simp [diff,eval] | coord i e => have h := HasDerivAt.comp_hasFDerivAt z (e.diff_correct (coordinateLinear i z)) (coordinateLinear i).hasFDerivAt have he : (.coord i e : BoxExpr).eval = e.eval ∘ coordinateLinear i := rfl rw [he, h.fderiv] by_cases hij : i=j · subst j simp only [diff, ↓reduceIte, eval, smul_apply, coordinateLinear_basis, smul_eq_mul, mul_one] · simp only [diff, eval, Rat.cast_zero, smul_apply, coordinateLinear_basis, ite_eq_right hij, smul_eq_mul, mul_zero] | add e f he hf => simp only [diff, eval, fderiv_fun_add (e.smooth.differentiable (by simp) z) (f.smooth.differentiable (by simp) z), add_apply, he, hf] | mul e f he hf => simp only [diff, eval, fderiv_fun_mul (e.smooth.differentiable (by simp) z) (f.smooth.differentiable (by simp) z), add_apply, smul_apply, smul_eq_mul, he, hf] ring def mixed (e : BoxExpr) : List (Fin 4) → BoxExpr | [] => e | j::α => (e.mixed α).diff j def bound : BoxExpr → ℚ → ℚ | .const q, _ => |q| | .coord _ e, R => e.bound R | .add e f, R => e.bound R + f.bound R | .mul e f, R => e.bound R * f.bound R theorem bound_nonneg (e : BoxExpr) (R : ℚ) : 0 ≤ e.bound R := by induction e with | const q => exact abs_nonneg q | coord i e => exact e.bound_nonneg R | add e f he hf => exact add_nonneg he hf | mul e f he hf => exact mul_nonneg he hf theorem bound_correct (e : BoxExpr) (R : ℚ) (z : SpaceTime) (hz : ∀ j, |flatten z j| ≤ |(R:ℝ)|) : |e.eval z| ≤ (e.bound R:ℝ) := by induction e with | const q => simp [eval,bound] | coord i e => exact e.bound_correct R (coordinateLinear i z) (by simpa using hz i) | add e f he hf => simpa only [eval,bound,Rat.cast_add] using (abs_add_le _ _).trans (add_le_add he hf) | mul e f he hf => simpa only [eval,bound,Rat.cast_mul,abs_mul] using mul_le_mul he hf (abs_nonneg _) (by exact_mod_cast e.bound_nonneg R) end BoxExpr def expressionField (e : Fin 3 → BoxExpr) : Field := fun t x j => (e j).eval (t,x) theorem expressionField_smooth (e : Fin 3 → BoxExpr) : Smooth (expressionField e) := contDiff_pi.mpr (fun j => (e j).smooth) theorem mixedDerivative_expressionField (e : Fin 3 → BoxExpr) (α : List (Fin 4)) : mixedDerivative (expressionField e) α = fun z j => ((e j).mixed α).eval z := by induction α with | nil => rfl | cons k α ih => ext z j rw [mixedDerivative,ih] change (fderiv ℝ (fun z j => ((e j).mixed α).eval z) z (spacetimeBasis k)) j = _ rw [fderiv_pi (fun i => ((e i).mixed α).smooth.differentiable (by simp) z)] exact (((e j).mixed α).diff_correct k z).symm def expressionBound (e : Fin 3 → BoxExpr) (α : List (Fin 4)) (R : ℚ) : ℚ := ∑ j, ((e j).mixed α).bound R theorem expressionBound_nonneg (e : Fin 3 → BoxExpr) (α : List (Fin 4)) (R : ℚ) : 0 ≤ expressionBound e α R := Finset.sum_nonneg (fun j _ => BoxExpr.bound_nonneg ((e j).mixed α) R) theorem expressionBound_correct (e : Fin 3 → BoxExpr) (α : List (Fin 4)) (R : ℚ) (z : SpaceTime) (hz : ∀ j, |flatten z j| ≤ |(R:ℝ)|) : ‖mixedDerivative (expressionField e) α z‖ ≤ (expressionBound e α R : ℝ) := by apply (pi_norm_le_iff_of_nonneg (by exact_mod_cast expressionBound_nonneg e α R)).mpr intro j rw [mixedDerivative_expressionField] change |((e j).mixed α).eval z| ≤ _ apply (BoxExpr.bound_correct _ R z hz).trans exact_mod_cast Finset.single_le_sum (fun i _ => BoxExpr.bound_nonneg _ _) (Finset.mem_univ j) def closedPeriodCell : Set SpaceTime := Set.Icc (0,0) (1,fun _ => 10) theorem mixedDerivative_eqOn_open {u v : Field} {S : Set SpaceTime} (hS : IsOpen S) (h : Set.EqOn (fun z => u z.1 z.2) (fun z => v z.1 z.2) S) (α : List (Fin 4)) : Set.EqOn (mixedDerivative u α) (mixedDerivative v α) S := by induction α with | nil => exact h | cons j α ih => intro z hz change fderiv ℝ (mixedDerivative u α) z (spacetimeBasis j) = _ rw [(ih.eventuallyEq_of_mem (hS.mem_nhds hz)).fderiv_eq] rfl theorem mixedDerivative_eqOn_cell {u v : Field} (hu : Smooth u) (hv : Smooth v) (h : Set.EqOn (fun z => u z.1 z.2) (fun z => v z.1 z.2) closedPeriodCell) (α : List (Fin 4)) : Set.EqOn (mixedDerivative u α) (mixedDerivative v α) closedPeriodCell := by have hc : Convex ℝ closedPeriodCell := convex_Icc _ _ have hn : (interior closedPeriodCell).Nonempty := by have he : interior closedPeriodCell = (Set.Ioo (0:ℝ) 1) ×ˢ (Set.pi Set.univ (fun _ : Fin 3 => Set.Ioo (0:ℝ) 10)) := by simp [closedPeriodCell, Set.Icc_prod_eq, interior_prod_eq, interior_Icc, ← Set.pi_univ_Icc, interior_pi_set] rw [he] exact ⟨(1/2,fun _ => 5), by norm_num [Set.mem_pi]⟩ have hi : Set.EqOn (mixedDerivative u α) (mixedDerivative v α) (interior closedPeriodCell) := mixedDerivative_eqOn_open isOpen_interior (h.mono interior_subset) α have hh := hi.closure (mixedDerivative_contDiff hu α).continuous (mixedDerivative_contDiff hv α).continuous have hclosure : closure (interior closedPeriodCell) = closedPeriodCell := hc.closure_interior_eq_closure_of_nonempty_interior hn |>.trans isClosed_Icc.closure_eq rwa [hclosure] at hh theorem periodic_expression_mixed_bound {u : Field} (hu : Smooth u) (hs : SpatiallyPeriodic u) (ht : OnePeriodic u) (e : Fin 3 → BoxExpr) (he : Set.EqOn (fun z => u z.1 z.2) (fun z => expressionField e z.1 z.2) closedPeriodCell) (α : List (Fin 4)) (z : SpaceTime) : ‖mixedDerivative u α z‖ ≤ (expressionBound e α 10 : ℝ) := by have hp := periodic_field_reduction (mixedDerivative_spatially_periodic hu hs α) (mixedDerivative_onePeriodic hu ht α) z.1 z.2 change mixedDerivative u α z = mixedDerivative u α (Int.fract z.1,wrapSpace z.2) at hp rw [hp] have hx : (Int.fract z.1,wrapSpace z.2) ∈ closedPeriodCell := ⟨⟨Int.fract_nonneg _, (wrapSpace_mem z.2).1⟩, ⟨(Int.fract_lt_one _).le, (wrapSpace_mem z.2).2⟩⟩ rw [mixedDerivative_eqOn_cell hu (expressionField_smooth e) he α hx] apply expressionBound_correct intro j fin_cases j · simp only [flatten, Rat.cast_ofNat, abs_of_pos (by norm_num : (0:ℝ)<10)] rw [abs_of_nonneg (Int.fract_nonneg _)] exact (Int.fract_lt_one _).le.trans (by norm_num) all_goals change |wrapSpace z.2 _| ≤ |(10:ℝ)| rw [abs_of_nonneg ((wrapSpace_mem z.2).1 _)] simpa using (wrapSpace_mem z.2).2 _ end Solenoidal end end OAI