import Mathlib import OAI.Analysis.CoulombIonization.RadialBounds.AnnularCellGeometryBarrier import OAI.Analysis.CoulombIonization.Localization.FiniteCellObservation namespace OAI noncomputable section namespace CoulombAtom section open MeasureTheory Filter Set open scoped BigOperators def SplitPositionSupport {N M : ℕ} (psi : FormVector (N+M)) (P Q : Space → Prop) : Prop := ∀ (s : Spins N) (t : Spins M) (x : Configuration N) (v : Configuration M), psi.value (joinLists s t) (joinLists x v) ≠ 0 → (∀ i, P (x i)) ∧ (∀ i, Q (v i)) lemma orderedCutForm_nonzero_factors {N : ℕ} (p : Fin 2 → SmoothMultiplier spaceDirections) (hp : ∀ x, ∑ a, (p a).value x^2=1) (psi : FormVector N) (c : Fin N → Fin 2) (s : Spins (cutCoreNumber c)) (t : Spins (cutOutNumber c)) (x : Configuration (cutCoreNumber c)) (v : Configuration (cutOutNumber c)) (hn : (orderedCutForm p hp psi c).value (joinLists s t) (joinLists x v) ≠ 0) : psi.value (joinLists s t ∘ (cutOrder c).symm) (joinLists x v ∘ (cutOrder c).symm) ≠ 0 ∧ (∀ i, (p 0).value (x i) ≠ 0) ∧ (∀ i, (p 1).value (v i) ≠ 0) := by have hv := hn rw [orderedCutForm_value] at hv change (spatialProductValue p (coreCutLabels (cutCoreNumber c) (cutOutNumber c)) (joinLists x v) : ℂ)*_ ≠ 0 at hv have hprod : spatialProductValue p (coreCutLabels (cutCoreNumber c) (cutOutNumber c)) (joinLists x v) ≠ 0 := by intro hh exact hv (by rw [hh,Complex.ofReal_zero,zero_mul]) refine ⟨(mul_ne_zero_iff.mp hv).2,?_,?_⟩ · intro i hi apply hprod apply Finset.prod_eq_zero (Finset.mem_univ (finSumFinEquiv (Sum.inl i))) simpa only [coreCutLabels,joinLists_left] using hi · intro i hi apply hprod apply Finset.prod_eq_zero (Finset.mem_univ (finSumFinEquiv (Sum.inr i))) simpa only [coreCutLabels,joinLists_right] using hi lemma SplitPositionSupport.observe {N M : ℕ} {psi : FormVector (N+M)} {P Q : Space → Prop} (hs : SplitPositionSupport psi P Q) (p : Fin 2 → SmoothMultiplier spaceDirections) (hp : ∀ x, ∑ a, (p a).value x^2=1) (hQ : ∀ z, (p 1).value z ≠ 0 → Q z) (c : Fin N → Fin 2) : SplitPositionSupport (nextCoreObservation p hp psi c) (fun z => P z ∧ (p 0).value z ≠ 0) Q := by intro s t x v hn have htn : t = joinLists (leftList t) (rightList t) := (join_list_parts t).symm have hvn : v = joinLists (leftList v) (rightList v) := (join_list_parts v).symm have hh : (orderedCutForm p hp (coreSlice psi (rightList t) (rightList v)) c).value (joinLists s (leftList t)) (joinLists x (leftList v)) ≠ 0 := by change (coreSlice (nextCoreObservation p hp psi c) t v).value s x ≠ 0 at hn conv at hn => lhs; arg 1; rw [htn,hvn,nextCoreObservation_slice] exact hn obtain ⟨hpsi,hcore,hout⟩ := orderedCutForm_nonzero_factors p hp _ c s (leftList t) x (leftList v) hh obtain ⟨hP,hQold⟩ := hs _ _ _ _ hpsi refine ⟨fun i => ⟨?_,hcore i⟩,?_⟩ · have hi := hP (cutOrder c (finSumFinEquiv (Sum.inl i))) simpa only [Function.comp_apply,Equiv.symm_apply_apply,joinLists_left] using hi · intro i obtain ⟨j,rfl⟩ := finSumFinEquiv.surjective i cases j with | inl j => exact hQ _ (hout j) | inr j => exact hQold j lemma SplitPositionSupport.mono {N M : ℕ} {psi : FormVector (N+M)} {P Q P' Q' : Space → Prop} (hs : SplitPositionSupport psi P Q) (hP : ∀ z, P z → P' z) (hQ : ∀ z, Q z → Q' z) : SplitPositionSupport psi P' Q' := by intro s t x v hn obtain ⟨hx,hv⟩ := hs s t x v hn exact ⟨fun i => hP _ (hx i),fun i => hQ _ (hv i)⟩ namespace CoreObservationGraph def supported (G : CoreObservationGraph) (P Q : Space → Prop) : Prop := SplitPositionSupport G.vector P Q lemma initial_supported {N : ℕ} (psi : FormVector N) (hpsi : SobolevFermion psi) (Q : Space → Prop) : (initial psi hpsi).supported (fun _ => True) Q := by intro s t x v hn exact ⟨fun _ => trivial,fun i => Fin.elim0 i⟩ lemma observe_supported (G : CoreObservationGraph) {P Q : Space → Prop} (hs : G.supported P Q) (p : Fin 2 → SmoothMultiplier spaceDirections) (hp : ∀ x, ∑ a, (p a).value x^2=1) (hQ : ∀ z, (p 1).value z ≠ 0 → Q z) (c : Fin G.coreSize → Fin 2) : (G.observe p hp c).supported (fun z => P z ∧ (p 0).value z ≠ 0) Q := hs.observe p hp hQ c end CoreObservationGraph namespace CoreObservationEnsemble def supported (E : CoreObservationEnsemble) (P Q : Space → Prop) : Prop := ∀ i, (E.graph i).supported P Q lemma initial_supported {N : ℕ} (psi : FormVector N) (hpsi : SobolevFermion psi) (Q : Space → Prop) : (initial psi hpsi).supported (fun _ => True) Q := fun _ => CoreObservationGraph.initial_supported psi hpsi Q lemma observe_supported (E : CoreObservationEnsemble) {P Q : Space → Prop} (hs : E.supported P Q) (p : Fin 2 → SmoothMultiplier spaceDirections) (hp : ∀ x, ∑ a, (p a).value x^2=1) (hQ : ∀ z, (p 1).value z ≠ 0 → Q z) : (E.observe p hp).supported (fun z => P z ∧ (p 0).value z ≠ 0) Q := fun ic => (hs ic.1).observe p hp hQ ic.2 end CoreObservationEnsemble end open MeasureTheory Set lemma cell_core_nonzero_distance {y z : Space} (hy : y ≠ 0) (hn : (coreFirstRadialCut y (localCellRadius_pos hy).le (localCellRadius_pos hy) 0).value z ≠ 0) : localCellRadius y ≤ ‖z-y‖ := by by_contra hh exact hn (coreFirstRadialCut_core_zero y (localCellRadius_pos hy).le (localCellRadius_pos hy) z hh) lemma cell_out_nonzero_norm {u : ℝ} (hu : 0 < u) {y z : Space} (hy : y ≠ 0) (hlo : u/2 ≤ ‖y‖) (hn : (coreFirstRadialCut y (localCellRadius_pos hy).le (localCellRadius_pos hy) 1).value z ≠ 0) : u/4 ≤ ‖z‖ := by have hd : ‖z-y‖ < localCellRadius y+localCellRadius y := by by_contra! hh exact hn (coreFirstRadialCut_out_zero y (localCellRadius_pos hy).le (localCellRadius_pos hy) z hh) have ht := norm_le_norm_sub_add y z rw [norm_sub_rev y z] at ht unfold localCellRadius at hd linarith namespace CoreObservationEnsemble lemma observeCells_supported (E : CoreObservationEnsemble) {P Q : Space → Prop} (hE : E.supported P Q) (ys : List Space) (hys : ∀ y ∈ ys, ∃ hy : y ≠ 0, ∀ z, (coreFirstRadialCut y (localCellRadius_pos hy).le (localCellRadius_pos hy) 1).value z ≠ 0 → Q z) : (E.observeCells ys).supported (fun z => P z ∧ ∀ y ∈ ys, localCellRadius y ≤ ‖z-y‖) Q := by induction ys generalizing E P with | nil => exact fun i => (hE i).mono (fun _ h => ⟨h,by simp⟩) (fun _ h => h) | cons y ys ih => obtain ⟨hy,hQ⟩ := hys y (List.mem_cons_self ..) have hs : (E.observeCell y).supported (fun z => P z ∧ localCellRadius y ≤ ‖z-y‖) Q := by rw [observeCell,dite_eq_right hy] intro i exact ((E.observe_supported hE _ _ hQ) i).mono (fun z h => ⟨h.1,cell_core_nonzero_distance hy h.2⟩) (fun _ h => h) have hh := ih _ hs (fun z hz => hys z (List.mem_cons_of_mem y hz)) intro i exact (hh i).mono (fun z h => ⟨h.1.1,fun w hw => by rcases List.mem_cons.mp hw with rfl | hw · exact h.1.2 · exact h.2 w hw⟩) (fun _ h => h) lemma annular_stencil_support {N : ℕ} (psi : FormVector N) (hpsi : SobolevFermion psi) {u : ℝ} (hu : 0 < u) (ys : List Space) (hys : ∀ y ∈ ys, u/2 ≤ ‖y‖) (hcover : ∀ z : Space, u/2 ≤ ‖z‖ → ‖z‖ ≤ 4*u → ∃ y ∈ ys, ‖z-y‖ < localCellRadius y) : ((initial psi hpsi).observeCells ys).supported (fun z => ¬(u/2 ≤ ‖z‖ ∧ ‖z‖ ≤ 4*u)) (fun z => u/4 ≤ ‖z‖) := by have hs := (initial psi hpsi).observeCells_supported (initial_supported psi hpsi (fun z => u/4 ≤ ‖z‖)) ys (by intro y hy have hn : y ≠ 0 := norm_pos_iff.mp (by linarith [hys y hy]) refine ⟨hn,fun z hz => cell_out_nonzero_norm hu hn (hys y hy) hz⟩) intro i exact (hs i).mono (fun z hz h => by obtain ⟨y,hy,hd⟩ := hcover z h.1 h.2 exact (not_lt_of_ge (hz.2 y hy)) hd) (fun _ h => h) end CoreObservationEnsemble lemma exists_scaled_shell_stencil : ∃ L : ℕ, ∀ u : ℝ, 0 < u → ∃ ys : List Space, ys.length = L ∧ (∀ y ∈ ys, u/2 ≤ ‖y‖ ∧ ‖y‖ ≤ 4*u) ∧ ∀ z : Space, u/2 ≤ ‖z‖ → ‖z‖ ≤ 4*u → ∃ y ∈ ys, ‖z-y‖ < localCellRadius y := by classical obtain ⟨T,hT,hcover⟩ := exists_annularCellStencil (by norm_num : (0:ℝ)<1/2) 4 refine ⟨T.card,fun u hu => ⟨(T.toList.map (fun v => u • v)),by simp,?_,?_⟩⟩ · intro y hy obtain ⟨v,hv,rfl⟩ := List.mem_map.mp hy have hvT := hT v (Finset.mem_toList.mp hv) rw [norm_smul,Real.norm_of_nonneg hu.le] constructor <;> nlinarith [hvT.1,hvT.2] · intro z hz hz4 obtain ⟨y,hy,hd⟩ := annularCell_scaled_cover hu T hcover (by linarith) hz4 obtain ⟨v,hv,rfl⟩ := Finset.mem_image.mp hy exact ⟨u • v,List.mem_map.mpr ⟨v,Finset.mem_toList.mpr hv,rfl⟩,hd⟩ end CoulombAtom end end OAI