import Mathlib import OAI.Analysis.CoulombIonization.FormDomain.WeakDerivativeSmulL2 import OAI.Analysis.CoulombIonization.FormDomain.GradientVector namespace OAI noncomputable section open MeasureTheory Filter open scoped Topology BigOperators ContDiff open MeasureTheory Filter Complex TopologicalSpace open scoped Topology InnerProductSpace ENNReal open MeasureTheory Filter Complex open scoped Topology BigOperators ComplexConjugate FourierTransform SchwartzMap ENNReal open MeasureTheory Filter open scoped Topology ContDiff SchwartzMap FourierTransform ENNReal open MeasureTheory Filter open scoped ContDiff InnerProductSpace Topology open MeasureTheory Filter open scoped ENNReal namespace CoulombAtom.Pauli open CoulombPauli CoulombPackets CoulombLT def oneParticleDensity {N : ℕ} (ψ : FormVector (N+1)) (hψ : ∀ s, MemLp (ψ.value s) 2) : Space → ℝ≥0∞ := fermionDensity (toMany ψ hψ) theorem form_lieb_thirring {N : ℕ} (ψ : FormVector (N+1)) (hψ : FormAdmissible ψ) : (∫⁻ x, oneParticleDensity ψ hψ.1 x ^ (5/3:ℝ)) ≤ ENNReal.ofReal (32*(N+1:ℝ) + (2048/3:ℝ)* (∑ s : Spins (N+1), ∑ i : Fin (N+1), ∑ a : Fin 3, ∫ x : Configuration (N+1), ‖ψ.gradient s i a x‖^2)) := by have hn : ‖toMany ψ hψ.1‖^2 = 1 := (toMany_norm_sq ψ hψ.1).trans hψ.2.2.2.2.1 have ha (i j : Fin (N+1)) (hij : i ≠ j) : permute (Equiv.swap i j) (toMany ψ hψ.1) = -toMany ψ hψ.1 := by rw [toMany_permute ψ hψ.1 (Equiv.swap i j) (hψ.2.2.2.1 _)] simp [Equiv.Perm.sign_swap hij] have hw (i : Fin (N+1)) (a : Fin 3) := form_hasFermionGradient ψ hψ i a simp only [EuclideanSpace.basisFun_apply] at hw have h := fermion_lieb_thirring (toMany ψ hψ.1) (gradientMany ψ hψ) hw hn ha simp only [gradientMany_norm_sq] at h have hs : (∑ s : Spins (N+1), ∑ i : Fin (N+1), ∑ a : Fin 3, ∫ x : Configuration (N+1), ‖ψ.gradient s i a x‖^2) = ∑ i : Fin (N+1), ∑ a : Fin 3, ∑ s : Spins (N+1), ∫ x : Configuration (N+1), ‖ψ.gradient s i a x‖^2 := by rw [Finset.sum_comm] exact Finset.sum_congr rfl (fun i _ => Finset.sum_comm) simpa only [oneParticleDensity,hs] using h end CoulombAtom.Pauli namespace CoulombLT open CoulombPauli CoulombPackets variable {V : Type*} [NormedAddCommGroup V] [InnerProductSpace ℝ V] [FiniteDimensional ℝ V] [MeasurableSpace V] [BorelSpace V] lemma coordinateDensity_aemeasurable {N : ℕ} (ψ : fermionL2 (V := V) (N+1)) (i : Fin (N+1)) : AEMeasurable (fun x => ∑ s : Fin 2, ∫⁻ y, ENNReal.ofReal (‖splitFermion i ψ ((x,s),y)‖^2) ∂(configMeasure N (spinSpaceMeasure (V := V)))) volume := by have hm := ((Lp.memLp (splitFermion i ψ)).aestronglyMeasurable.norm.pow 2).aemeasurable.ennreal_ofReal have h1 := hm.lintegral_prod_right' have h2 := h1.lintegral_prod_right' simpa only [lintegral_fintype,Measure.count_singleton,mul_one,Pi.pow_apply] using h2 lemma fermionDensity_aemeasurable {N : ℕ} (ψ : fermionL2 (V := V) (N+1)) : AEMeasurable (fermionDensity ψ) volume := by exact Finset.aemeasurable_fun_sum Finset.univ (fun i _ => coordinateDensity_aemeasurable ψ i) lemma coordinate_density_weighted {N : ℕ} (ψ : fermionL2 (V := V) (N+1)) (i : Fin (N+1)) (w : V → ℝ) (hw : Measurable w) : (∫⁻ x, ENNReal.ofReal (w x) * (∑ s : Fin 2, ∫⁻ y, ENNReal.ofReal (‖splitFermion i ψ ((x,s),y)‖^2) ∂(configMeasure N (spinSpaceMeasure (V := V))))) = ∫⁻ q, ENNReal.ofReal (w (q i).1) * ENNReal.ofReal (‖ψ q‖^2) ∂(configMeasure (N+1) (spinSpaceMeasure (V := V))) := by let ν := configMeasure N (spinSpaceMeasure (V := V)) have hm : AEMeasurable (fun p : (V × Fin 2) × (Fin N → V × Fin 2) => ENNReal.ofReal (w p.1.1) * ENNReal.ofReal (‖splitFermion i ψ p‖^2)) ((spinSpaceMeasure (V := V)).prod ν) := ((hw.comp (measurable_fst.comp measurable_fst)).ennreal_ofReal.aemeasurable).mul ((Lp.memLp (splitFermion i ψ)).aestronglyMeasurable.norm.pow 2).aemeasurable.ennreal_ofReal have hp := splitAt_preserving (μ := spinSpaceMeasure (V := V)) i have ha := pull_ae (splitAt i).symm (hp.symm (splitAt i)) ψ calc _ = ∫⁻ x, ∫⁻ s : Fin 2, ∫⁻ y, ENNReal.ofReal (w x) * ENNReal.ofReal (‖splitFermion i ψ ((x,s),y)‖^2) ∂ν ∂Measure.count := by apply lintegral_congr intro x simp only [lintegral_const_mul' _ _ ENNReal.ofReal_ne_top,lintegral_fintype,Measure.count_singleton,mul_one,Finset.mul_sum] rfl _ = ∫⁻ p, ENNReal.ofReal (w p.1.1) * ENNReal.ofReal (‖splitFermion i ψ p‖^2) ∂((spinSpaceMeasure (V := V)).prod ν) := by rw [lintegral_prod _ hm,lintegral_prod _ hm.lintegral_prod_right'] _ = ∫⁻ p, ENNReal.ofReal (w p.1.1) * ENNReal.ofReal (‖ψ ((splitAt i).symm p)‖^2) ∂((spinSpaceMeasure (V := V)).prod ν) := by apply lintegral_congr_ae filter_upwards [ha] with p hp rw [← hp] rfl _ = _ := by have he := (hp.symm (splitAt i)).lintegral_comp_emb (splitAt i).symm.measurableEmbedding (fun q => ENNReal.ofReal (w (q i).1) * ENNReal.ofReal (‖ψ q‖^2)) have hs (p : (V × Fin 2) × (Fin N → V × Fin 2)) : (splitAt i).symm p i = p.1 := by exact congrArg Prod.fst ((splitAt i).apply_symm_apply p) simp_rw [hs] at he exact he lemma density_weighted_lintegral {N : ℕ} (ψ : fermionL2 (V := V) (N+1)) (w : V → ℝ) (hw : Measurable w) : (∫⁻ x, ENNReal.ofReal (w x) * fermionDensity ψ x) = ∑ i : Fin (N+1), ∫⁻ q, ENNReal.ofReal (w (q i).1) * ENNReal.ofReal (‖ψ q‖^2) ∂(configMeasure (N+1) (spinSpaceMeasure (V := V))) := by change (∫⁻ x, ENNReal.ofReal (w x) * ∑ i : Fin (N+1), ∑ s : Fin 2, ∫⁻ y, ENNReal.ofReal (‖splitFermion i ψ ((x,s),y)‖^2) ∂(configMeasure N (spinSpaceMeasure (V := V)))) = _ conv_lhs => arg 2; ext x; rw [Finset.mul_sum] rw [lintegral_finsetSum' (f := fun i x => ENNReal.ofReal (w x) * (∑ s : Fin 2, ∫⁻ y, ENNReal.ofReal (‖splitFermion i ψ ((x,s),y)‖^2) ∂(configMeasure N (spinSpaceMeasure (V := V))))) Finset.univ (fun i _ => hw.ennreal_ofReal.aemeasurable.mul (coordinateDensity_aemeasurable ψ i))] exact Finset.sum_congr rfl (fun i _ => coordinate_density_weighted ψ i w hw) end CoulombLT end end OAI