import Mathlib import OAI.Analysis.CoulombIonization.Model import OAI.Analysis.CoulombIonization.FormDomain.WeakDerivative namespace OAI noncomputable section open MeasureTheory Filter open scoped Topology BigOperators ContDiff open MeasureTheory Filter open scoped Topology BigOperators ContDiff InnerProductSpace Convolution namespace CoulombAtom section WeakChangeVariables variable {E : Type*} [NormedAddCommGroup E] [NormedSpace ℝ E] [FiniteDimensional ℝ E] [MeasureSpace E] [BorelSpace E] omit [FiniteDimensional ℝ E] in lemma IsWeakDerivative.comp_linearEquiv {v w : E} {f g : E → ℂ} (hw : IsWeakDerivative v f g) (e : E ≃L[ℝ] E) (he : MeasurePreserving e) (hv : e w = v) : IsWeakDerivative w (f ∘ e) (g ∘ e) := by intro φ hφ hcφ let ψ : E → ℝ := φ ∘ e.symm have hψ : ContDiff ℝ ∞ ψ := hφ.comp e.symm.contDiff have hcψ : HasCompactSupport ψ := hcφ.comp_homeomorph e.symm.toHomeomorph have hev : e.symm v = w := by rw [← hv, e.symm_apply_apply] have hd (x : E) : lineDeriv ℝ ψ (e x) v = lineDeriv ℝ φ x w := by rw [(hψ.differentiable (by simp) (e x)).lineDeriv_eq_fderiv, (hφ.differentiable (by simp) x).lineDeriv_eq_fderiv] have hh := (hφ.differentiable (by simp) (e.symm (e x))).hasFDerivAt.comp (e x) (e.symm.hasFDerivAt) have hh' := congrArg (fun A : E →L[ℝ] ℝ => A v) hh.fderiv simpa only [ContinuousLinearMap.comp_apply, ContinuousLinearEquiv.coe_coe, e.symm_apply_apply, hev] using hh' have hi1 : (∫ x, f (e x) * Complex.ofReal (lineDeriv ℝ ψ (e x) v)) = ∫ x, f x * Complex.ofReal (lineDeriv ℝ ψ x v) := he.integral_comp e.toHomeomorph.measurableEmbedding (fun x => f x * Complex.ofReal (lineDeriv ℝ ψ x v)) have hi2 : (∫ x, g (e x) * (ψ (e x) : ℂ)) = ∫ x, g x * (ψ x : ℂ) := he.integral_comp e.toHomeomorph.measurableEmbedding (fun x => g x * (ψ x : ℂ)) have hh := hw ψ hψ hcψ rw [← hi1, ← hi2] at hh simpa only [hd, ψ, Function.comp_apply, e.symm_apply_apply] using hh end WeakChangeVariables section WeakGraphChange variable {E : Type*} [NormedAddCommGroup E] [NormedSpace ℝ E] [FiniteDimensional ℝ E] [MeasureSpace E] [BorelSpace E] [IsLocallyFiniteMeasure (volume : Measure E)] variable {ι : Type*} [Fintype ι] def weakGraphChangeAmbient (v : ι → E) (e : E ≃L[ℝ] E) (he : MeasurePreserving e) (κ : ι → ι) : weakGraph v →L[ℂ] WeakGraphAmbient E ι := (PiLp.continuousLinearEquiv 2 ℂ (fun _ : Option ι => Lp ℂ 2 (volume : Measure E)) ).symm.toContinuousLinearMap.comp (ContinuousLinearMap.pi fun j => (Lp.compMeasurePreservingₗᵢ ℂ e he).toContinuousLinearMap.comp ((PiLp.proj 2 (fun _ : Option ι => Lp ℂ 2 (volume : Measure E)) (j.map κ)).comp (weakGraph v).subtypeL)) omit [Fintype ι] in lemma weakGraphChangeAmbient_mem (v : ι → E) (e : E ≃L[ℝ] E) (he : MeasurePreserving e) (κ : ι → ι) (hv : ∀ i, e (v i) = v (κ i)) (F : weakGraph v) : weakGraphChangeAmbient v e he κ F ∈ weakGraph v := by rw [mem_weakGraph] intro i have hh := ((mem_weakGraph v F.val).mp F.property (κ i)).comp_linearEquiv e he (hv i) exact hh.congr_ae (Lp.coeFn_compMeasurePreserving (F.val none) he).symm (Lp.coeFn_compMeasurePreserving (F.val (some (κ i))) he).symm def weakGraphChange (v : ι → E) (e : E ≃L[ℝ] E) (he : MeasurePreserving e) (κ : ι → ι) (hv : ∀ i, e (v i) = v (κ i)) : weakGraph v →L[ℂ] weakGraph v := (weakGraphChangeAmbient v e he κ).codRestrict (weakGraph v) (weakGraphChangeAmbient_mem v e he κ hv) end WeakGraphChange abbrev SectorHilbert (N : ℕ) := PiLp 2 (fun _ : Spins N => Lp ℂ 2 (volume : Measure (Configuration N))) def permuteConfiguration {N : ℕ} (π : Equiv.Perm (Fin N)) : Configuration N ≃L[ℝ] Configuration N := ContinuousLinearEquiv.piCongrLeft ℝ (fun _ : Fin N => Space) π.symm @[simp] lemma permuteConfiguration_apply {N : ℕ} (π : Equiv.Perm (Fin N)) (x : Configuration N) : permuteConfiguration π x = x ∘ π := by ext i simp [permuteConfiguration, ContinuousLinearEquiv.piCongrLeft, Equiv.piCongrLeft] lemma permuteConfiguration_preserving {N : ℕ} (π : Equiv.Perm (Fin N)) : MeasurePreserving (permuteConfiguration π) := by exact volume_measurePreserving_piCongrLeft (fun _ : Fin N => Space) π.symm def fermionPermutation {N : ℕ} (π : Equiv.Perm (Fin N)) : SectorHilbert N →L[ℂ] SectorHilbert N := (PiLp.continuousLinearEquiv 2 ℂ (fun _ : Spins N => Lp ℂ 2 (volume : Measure (Configuration N))) ).symm.toContinuousLinearMap.comp (ContinuousLinearMap.pi fun s => ((((Equiv.Perm.sign π : ℤ) : ℂ)) • (Lp.compMeasurePreservingₗᵢ ℂ (permuteConfiguration π) (permuteConfiguration_preserving π)).toContinuousLinearMap).comp (PiLp.proj 2 (fun _ : Spins N => Lp ℂ 2 (volume : Measure (Configuration N))) (s ∘ π))) def fermionSpace (N : ℕ) : Submodule ℂ (SectorHilbert N) := ⨅ π : Equiv.Perm (Fin N), (fermionPermutation π - ContinuousLinearMap.id ℂ _).ker lemma mem_fermionSpace {N : ℕ} (F : SectorHilbert N) : F ∈ fermionSpace N ↔ ∀ π : Equiv.Perm (Fin N), fermionPermutation π F = F := by simp [fermionSpace, sub_eq_zero] lemma fermionSpace_isClosed (N : ℕ) : IsClosed (fermionSpace N : Set (SectorHilbert N)) := by simp only [fermionSpace, Submodule.coe_iInf] exact isClosed_iInter fun π => (fermionPermutation π - ContinuousLinearMap.id ℂ _).isClosed_ker instance fermionSpace_completeSpace (N : ℕ) : CompleteSpace (fermionSpace N) := (fermionSpace_isClosed N).completeSpace_coe abbrev sectorDirections (N : ℕ) : Fin N × Fin 3 → Configuration N := fun k => direction k.1 k.2 instance weakSectorGraph_normedAddCommGroup (N : ℕ) : NormedAddCommGroup (weakGraph (sectorDirections N)) := Submodule.normedAddCommGroup _ instance weakSectorGraph_innerProductSpace (N : ℕ) : InnerProductSpace ℂ (weakGraph (sectorDirections N)) := Submodule.innerProductSpace _ instance weakSectorGraph_normedSpace (N : ℕ) : NormedSpace ℂ (weakGraph (sectorDirections N)) := Submodule.normedSpace _ abbrev SectorGraph (N : ℕ) := PiLp 2 (fun _ : Spins N => weakGraph (sectorDirections N)) instance sectorGraph_normedAddCommGroup (N : ℕ) : NormedAddCommGroup (SectorGraph N) := PiLp.normedAddCommGroup 2 _ instance sectorGraph_innerProductSpace (N : ℕ) : InnerProductSpace ℂ (SectorGraph N) := PiLp.innerProductSpace _ instance sectorGraph_normedSpace (N : ℕ) : NormedSpace ℂ (SectorGraph N) := PiLp.normedSpace 2 ℂ _ def sectorGraphValue (N : ℕ) : SectorGraph N →L[ℂ] SectorHilbert N := (PiLp.continuousLinearEquiv 2 ℂ (fun _ : Spins N => Lp ℂ 2 (volume : Measure (Configuration N))) ).symm.toContinuousLinearMap.comp (ContinuousLinearMap.pi fun s => (weakGraphValue (sectorDirections N)).comp (PiLp.proj 2 (fun _ : Spins N => weakGraph (sectorDirections N)) s)) @[simp] lemma sectorGraphValue_apply {N : ℕ} (F : SectorGraph N) (s : Spins N) : sectorGraphValue N F s = (F s).val none := rfl lemma sectorGraphValue_injective (N : ℕ) : Function.Injective (sectorGraphValue N) := by intro F G hFG apply PiLp.ext intro s apply weakGraphValue_injective (sectorDirections N) exact congrArg (fun h : SectorHilbert N => h s) hFG def fermionGraph (N : ℕ) : Submodule ℂ (SectorGraph N) := (fermionSpace N).comap (sectorGraphValue N).toLinearMap instance fermionGraph_normedAddCommGroup (N : ℕ) : NormedAddCommGroup (fermionGraph N) := Submodule.normedAddCommGroup _ instance fermionGraph_innerProductSpace (N : ℕ) : InnerProductSpace ℂ (fermionGraph N) := Submodule.innerProductSpace _ instance fermionGraph_normedSpace (N : ℕ) : NormedSpace ℂ (fermionGraph N) := Submodule.normedSpace _ lemma fermionGraph_isClosed (N : ℕ) : IsClosed (fermionGraph N : Set (SectorGraph N)) := (fermionSpace_isClosed N).preimage (sectorGraphValue N).continuous instance fermionGraph_completeSpace (N : ℕ) : CompleteSpace (fermionGraph N) := (fermionGraph_isClosed N).completeSpace_coe def fermionGraphValue (N : ℕ) : fermionGraph N →L[ℂ] fermionSpace N := ((sectorGraphValue N).comp (fermionGraph N).subtypeL).codRestrict (fermionSpace N) (fun F => F.property) lemma fermionGraphValue_injective (N : ℕ) : Function.Injective (fermionGraphValue N) := by intro F G hFG apply Subtype.ext apply sectorGraphValue_injective N exact congrArg Subtype.val hFG end CoulombAtom end end OAI