import Mathlib import OAI.Analysis.CoulombIonization.FieldAnalysis.InnerFieldCap import OAI.Analysis.CoulombIonization.RadialBounds.CoulombTailStatistic namespace OAI noncomputable section namespace CoulombAtom section open MeasureTheory Filter Set open scoped BigOperators def innerFieldVolume (h : ℝ) : ℝ := volume.real (innerFieldTestAnnulus h) lemma innerFieldVolume_nonneg (h : ℝ) : 0 ≤ innerFieldVolume h := measureReal_nonneg lemma positiveCoreField_annular_sq_integrable {N : ℕ} {psi : FormVector N} (hpsi : SobolevVector psi) {Z lam h : ℝ} (hZ : 0 ≤ Z) (hlam : 0 ≤ lam) (hh : 0 < h) : IntegrableOn (fun z => (max (normalizedCoreField Z lam psi z) 0)^2) (innerFieldTestAnnulus h) := by let : IsFiniteMeasure (volume.restrict (innerFieldTestAnnulus h)) := ⟨by rw [Measure.restrict_apply_univ]; exact innerFieldTestAnnulus_finite h⟩ apply (integrable_const ((Z/h)^2)).mono' (((normalizedCoreField_measurable hpsi Z lam).max measurable_const).pow_const 2).aestronglyMeasurable filter_upwards [ae_restrict_mem (innerFieldTestAnnulus_measurable h)] with z hz rw [Real.norm_of_nonneg (sq_nonneg _)] exact pow_le_pow_left₀ (le_max_right _ _) (normalizedCoreField_pos_le psi hZ hlam hh hz.1) 2 lemma positiveCoreField_annular_cauchy {N : ℕ} {psi : FormVector N} (hpsi : SobolevVector psi) {Z lam h : ℝ} (hZ : 0 ≤ Z) (hlam : 0 ≤ lam) (hh : 0 < h) : (∫ z in innerFieldTestAnnulus h, max (normalizedCoreField Z lam psi z) 0)^2 ≤ innerFieldVolume h*(∫ z in innerFieldTestAnnulus h, (max (normalizedCoreField Z lam psi z) 0)^2) := by let mu := volume.restrict (innerFieldTestAnnulus h) let : IsFiniteMeasure mu := ⟨by rw [Measure.restrict_apply_univ]; exact innerFieldTestAnnulus_finite h⟩ let f := fun z => max (normalizedCoreField Z lam psi z) 0 have h1 : Integrable f mu := positiveCoreField_annular_integrable hpsi hZ hlam hh have h2 : Integrable (fun z => f z^2) mu := positiveCoreField_annular_sq_integrable hpsi hZ hlam hh have hc := weighted_sum_integral_cauchy (fun _ : Unit => mu) (fun _ _ => (1:ℝ)) (fun _ z => f z) (fun _ _ => (1:ℝ)) (fun _ _ => zero_le_one) (fun _ => by simpa only [mul_one] using h2) (fun _ => by simpa only [one_pow,one_mul] using (integrable_const (1:ℝ) : Integrable (fun _ : Space => (1:ℝ)) mu)) (fun _ => by simpa only [mul_one] using h1) simp only [Finset.univ_unique,Finset.sum_singleton,mul_one,one_pow,integral_const, smul_eq_mul,Measure.real] at hc have hsq := pow_le_pow_left₀ (integral_nonneg (fun z => le_max_right _ _)) hc 2 rw [mul_pow,Real.sq_sqrt (integral_nonneg (fun z => sq_nonneg _)), Real.sq_sqrt (by dsimp [mu]; positivity)] at hsq simpa only [f,mu,innerFieldVolume,Measure.real,Measure.restrict_apply_univ,mul_comm] using hsq def innerCapStatistic {N : ℕ} (psi : FormVector N) (Z lam h : ℝ) : ℝ := 3*(packetDensityConstant/(h/4)^3)^2*innerFieldVolume h* (∫ z in innerFieldTestAnnulus h, coreFieldSquare Z lam z psi)+ 3*lam^2*formMass psi+3*(16*packetPotentialConstant)^2*rawWeightedMoment psi (coulombTailWeight h) lemma innerCapStatistic_nonneg {N : ℕ} (psi : FormVector N) (Z lam h : ℝ) : 0 ≤ innerCapStatistic psi Z lam h := by unfold innerCapStatistic have hv := innerFieldVolume_nonneg h have hf : 0 ≤ ∫ z in innerFieldTestAnnulus h, coreFieldSquare Z lam z psi := integral_nonneg (fun z => coreFieldSquare_nonneg Z lam z psi) have hm := formMass_nonneg psi have ht := rawWeightedMoment_nonneg psi (coulombTailWeight h) positivity theorem actualInnerBoundaryCap_sq_le_statistic {N : ℕ} {psi : FormVector N} (hpsi : SobolevVector psi) {Z lam h : ℝ} (hZ : 0 ≤ Z) (hlam : 0 ≤ lam) (hh : 0 < h) : (actualInnerBoundaryCap psi Z lam h)^2*formMass psi ≤ innerCapStatistic psi Z lam h := by let A := packetDensityConstant/(h/4)^3 let B := 16*packetPotentialConstant let U := ∫ z in innerFieldTestAnnulus h, max (normalizedCoreField Z lam psi z) 0 let T := ∫ a, ‖a‖⁻¹ ∂(actualParticleSource psi).restrict {a | h < ‖a‖} let M := formMass psi have hM : 0 ≤ M := formMass_nonneg psi have hU := mul_le_mul_of_nonneg_right (positiveCoreField_annular_cauchy hpsi hZ hlam hh) hM have hT := actual_tail_square_le hpsi hh have hx : (A*U+lam+B*T)^2 ≤ 3*((A*U)^2+lam^2+(B*T)^2) := by nlinarith only [sq_nonneg (A*U-lam),sq_nonneg (A*U-B*T),sq_nonneg (lam-B*T)] have hxm := mul_le_mul_of_nonneg_right hx hM have he : (∫ z in innerFieldTestAnnulus h, coreFieldSquare Z lam z psi) = (∫ z in innerFieldTestAnnulus h, (max (normalizedCoreField Z lam psi z) 0)^2)*M := by exact integral_mul_const M _ unfold actualInnerBoundaryCap innerCapStatistic rw [he] change (A*U+lam+B*T)^2*M ≤ 3*A^2*innerFieldVolume h*((∫ z in innerFieldTestAnnulus h, (max (normalizedCoreField Z lam psi z) 0)^2)*M)+ 3*lam^2*M+3*B^2*rawWeightedMoment psi (coulombTailWeight h) have h1 := mul_le_mul_of_nonneg_left hU (show 0 ≤ 3*A^2 by positivity) have h2 := mul_le_mul_of_nonneg_left hT (show 0 ≤ 3*B^2 by positivity) nlinarith only [hxm,h1,h2] theorem actual_inner_exterior_sq_statistic {N : ℕ} {psi : FormVector N} (hpsi : SobolevVector psi) (hm : formMass psi ≠ 0) {Z lam h : ℝ} (hZ : 0 ≤ Z) (hlam : 0 ≤ lam) (hh : 0 < h) {y : Space} (hy : 2*h ≤ ‖y‖) : (max (sourceField Z (actualInnerSource psi h) y) 0)^2*formMass psi ≤ innerCapStatistic psi Z lam h*((2*h)/‖y‖)^2 := by have hcap := actual_inner_exterior_cap hpsi hm hZ hlam hh hy have hc := actualInnerBoundaryCap_nonneg psi Z hlam hh have hq : 0 ≤ (2*h)/‖y‖ := by positivity have hf : max (sourceField Z (actualInnerSource psi h) y) 0 ≤ actualInnerBoundaryCap psi Z lam h*((2*h)/‖y‖) := by apply max_le · simpa only [mul_div_assoc] using hcap · exact mul_nonneg hc hq have hp := mul_le_mul_of_nonneg_right (pow_le_pow_left₀ (le_max_right _ _) hf 2) (formMass_nonneg psi) calc _ ≤ (actualInnerBoundaryCap psi Z lam h*((2*h)/‖y‖))^2*formMass psi := hp _ = (actualInnerBoundaryCap psi Z lam h)^2*formMass psi*((2*h)/‖y‖)^2 := by ring _ ≤ _ := mul_le_mul_of_nonneg_right (actualInnerBoundaryCap_sq_le_statistic hpsi hZ hlam hh) (sq_nonneg _) end open MeasureTheory Filter Set Metric open scoped BigOperators def innerFieldAnnulusWeight (h : ℝ) : Space → ℝ := (innerFieldTestAnnulus h).indicator (fun _ => 1) lemma innerFieldAnnulusWeight_integrable (h : ℝ) : Integrable (innerFieldAnnulusWeight h) := by rw [innerFieldAnnulusWeight,integrable_indicator_iff (innerFieldTestAnnulus_measurable h)] exact integrableOn_const (C := (1:ℝ)) (hs := innerFieldTestAnnulus_finite h |>.ne) lemma innerFieldAnnulusWeight_nonneg (h : ℝ) (z : Space) : 0 ≤ innerFieldAnnulusWeight h z := indicator_nonneg (fun _ _ => zero_le_one) z lemma innerFieldAnnulusWeight_separation (h : ℝ) (z : Space) (hz : innerFieldAnnulusWeight h z ≠ 0) : h ≤ ‖z‖ := by by_contra! hc exact hz (indicator_of_notMem (by intro hd; exact (not_le_of_gt hc) hd.1) _) lemma innerFieldAnnulus_weight_eq (h : ℝ) (f : Space → ℝ) : (∫ z, f z*innerFieldAnnulusWeight h z) = ∫ z in innerFieldTestAnnulus h, f z := by rw [←integral_indicator (innerFieldTestAnnulus_measurable h)] apply integral_congr_ae exact ae_of_all _ (fun z => by by_cases hz : z ∈ innerFieldTestAnnulus h <;> simp [innerFieldAnnulusWeight,hz]) lemma coreFieldSquare_annular_statistic_integrable {N M : ℕ} {ψ : FormVector (N+M)} (hψ : SobolevVector ψ) (t : Spins M) {Z lam h : ℝ} (hZ : 0 ≤ Z) (hlam : 0 ≤ lam) (hh : 0 < h) : Integrable (fun u => ∫ z in innerFieldTestAnnulus h, coreFieldSquare Z lam z (coreSlice ψ t u)) := by have hi := (coreFieldSquare_weighted_prod_integrable hψ t hZ hlam hh (innerFieldAnnulusWeight_integrable h) (innerFieldAnnulusWeight_nonneg h) (innerFieldAnnulusWeight_separation h)).integral_prod_left simpa only [innerFieldAnnulus_weight_eq] using hi lemma coreFieldSquare_annular_fubini {N M : ℕ} {ψ : FormVector (N+M)} (hψ : SobolevVector ψ) {Z lam h : ℝ} (hZ : 0 ≤ Z) (hlam : 0 ≤ lam) (hh : 0 < h) : coreLawAverage ψ (fun φ => ∫ z in innerFieldTestAnnulus h, coreFieldSquare Z lam z φ) = ∫ z in innerFieldTestAnnulus h, coreLawAverage ψ (coreFieldSquare Z lam z) := by have he := coreFieldSquare_weighted_fubini hψ Z lam hZ hlam hh (innerFieldAnnulusWeight_integrable h) (innerFieldAnnulusWeight_nonneg h) (innerFieldAnnulusWeight_separation h) simpa only [innerFieldAnnulus_weight_eq] using he lemma innerCapStatistic_coreSlice_integrable {N M : ℕ} {ψ : FormVector (N+M)} (hψ : SobolevVector ψ) (t : Spins M) {Z lam h : ℝ} (hZ : 0 ≤ Z) (hlam : 0 ≤ lam) (hh : 0 < h) : Integrable (fun u => innerCapStatistic (coreSlice ψ t u) Z lam h) := by unfold innerCapStatistic exact (((coreFieldSquare_annular_statistic_integrable hψ t hZ hlam hh).const_mul _).add ((hψ.coreSlice_mass_integrable t).const_mul _)).add ((rawWeightedMoment_coreSlice_integrable hψ (coulombTailWeight_measurable h) (coulombTailWeight_nonneg h) (coulombTailWeight_le hh) t).const_mul _) namespace CoreObservationGraph def innerCapAverage (G : CoreObservationGraph) (Z lam h : ℝ) : ℝ := coreLawAverage G.vector (fun φ => innerCapStatistic φ Z lam h) lemma fieldMoment_annular_integrable (G : CoreObservationGraph) {Z lam h : ℝ} (hZ : 0 ≤ Z) (hlam : 0 ≤ lam) (hh : 0 < h) : IntegrableOn (G.fieldMoment Z lam) (innerFieldTestAnnulus h) := by have hi := G.fieldMoment_weighted_integrable hZ hlam hh (innerFieldAnnulusWeight_integrable h) (innerFieldAnnulusWeight_nonneg h) (innerFieldAnnulusWeight_separation h) rw [←integrable_indicator_iff (innerFieldTestAnnulus_measurable h)] apply hi.congr exact ae_of_all _ (fun z => by by_cases hz : z ∈ innerFieldTestAnnulus h <;> simp [innerFieldAnnulusWeight,hz]) lemma innerCapAverage_eq (G : CoreObservationGraph) {Z lam h : ℝ} (hZ : 0 ≤ Z) (hlam : 0 ≤ lam) (hh : 0 < h) : G.innerCapAverage Z lam h = 3*(packetDensityConstant/(h/4)^3)^2*innerFieldVolume h* (∫ z in innerFieldTestAnnulus h, G.fieldMoment Z lam z)+ 3*lam^2*G.mass+3*(16*packetPotentialConstant)^2*G.weightedMoment (coulombTailWeight h) := by have he : G.innerCapAverage Z lam h = 3*(packetDensityConstant/(h/4)^3)^2*innerFieldVolume h* coreLawAverage G.vector (fun φ => ∫ z in innerFieldTestAnnulus h, coreFieldSquare Z lam z φ)+ 3*lam^2*coreLawAverage G.vector formMass+ 3*(16*packetPotentialConstant)^2*G.weightedMoment (coulombTailWeight h) := by unfold innerCapAverage coreLawAverage innerCapStatistic weightedMoment coreLawAverage rw [Finset.mul_sum,Finset.mul_sum,Finset.mul_sum,←Finset.sum_add_distrib,←Finset.sum_add_distrib] apply Finset.sum_congr rfl intro t _ dsimp only have hA : Integrable (fun v => 3*(packetDensityConstant/(h/4)^3)^2*innerFieldVolume h* (∫ z in innerFieldTestAnnulus h, coreFieldSquare Z lam z (coreSlice G.vector t v))) := (coreFieldSquare_annular_statistic_integrable G.sobolev t hZ hlam hh).const_mul _ have hB : Integrable (fun v => 3*lam^2*formMass (coreSlice G.vector t v)) := (G.sobolev.coreSlice_mass_integrable t).const_mul _ have hC : Integrable (fun v => 3*(16*packetPotentialConstant)^2* rawWeightedMoment (coreSlice G.vector t v) (coulombTailWeight h)) := (rawWeightedMoment_coreSlice_integrable G.sobolev (coulombTailWeight_measurable h) (coulombTailWeight_nonneg h) (coulombTailWeight_le hh) t).const_mul _ have hAB := integral_add hA hB have hABC := integral_add (hA.add hB) hC simp only [Pi.add_apply] at hABC hAB rw [hABC,hAB] simp only [integral_const_mul] rw [he,coreFieldSquare_annular_fubini G.sobolev hZ hlam hh,coreLawAverage_mass G.sobolev] rfl end CoreObservationGraph namespace CoreObservationEnsemble def innerCapAverage (E : CoreObservationEnsemble) (Z lam h : ℝ) : ℝ := ∑ i, (E.graph i).innerCapAverage Z lam h lemma fieldMoment_annular_integrable (E : CoreObservationEnsemble) {Z lam h : ℝ} (hZ : 0 ≤ Z) (hlam : 0 ≤ lam) (hh : 0 < h) : IntegrableOn (E.fieldMoment Z lam) (innerFieldTestAnnulus h) := integrable_finsetSum _ (fun i _ => (E.graph i).fieldMoment_annular_integrable hZ hlam hh) lemma innerCapAverage_eq (E : CoreObservationEnsemble) {Z lam h : ℝ} (hZ : 0 ≤ Z) (hlam : 0 ≤ lam) (hh : 0 < h) : E.innerCapAverage Z lam h = 3*(packetDensityConstant/(h/4)^3)^2*innerFieldVolume h* (∫ z in innerFieldTestAnnulus h, E.fieldMoment Z lam z)+ 3*lam^2*E.mass+3*(16*packetPotentialConstant)^2*E.weightedMoment (coulombTailWeight h) := by unfold innerCapAverage simp_rw [CoreObservationGraph.innerCapAverage_eq _ hZ hlam hh] simp only [Finset.sum_add_distrib,←Finset.mul_sum] unfold fieldMoment mass weightedMoment rw [integral_finsetSum _ (fun i _ => (E.graph i).fieldMoment_annular_integrable hZ hlam hh)] lemma innerCapAverage_bound (E : CoreObservationEnsemble) {Z lam h F T : ℝ} (hZ : 0 ≤ Z) (hlam : 0 ≤ lam) (hh : 0 < h) (hm : E.mass = 1) (hf : ∀ z ∈ innerFieldTestAnnulus h, E.fieldMoment Z lam z ≤ F) (ht : E.weightedMoment (coulombTailWeight h) ≤ T) : E.innerCapAverage Z lam h ≤ 3*(packetDensityConstant/(h/4)^3)^2*(innerFieldVolume h)^2*F+ 3*lam^2+3*(16*packetPotentialConstant)^2*T := by rw [innerCapAverage_eq E hZ hlam hh,hm,mul_one] have hI : (∫ z in innerFieldTestAnnulus h, E.fieldMoment Z lam z) ≤ innerFieldVolume h*F := by let : IsFiniteMeasure (volume.restrict (innerFieldTestAnnulus h)) := ⟨by rw [Measure.restrict_apply_univ]; exact innerFieldTestAnnulus_finite h⟩ have hb := integral_mono_ae (E.fieldMoment_annular_integrable hZ hlam hh) (integrable_const F) (ae_restrict_of_forall_mem (innerFieldTestAnnulus_measurable h) hf) simpa only [integral_const,Measure.real,Measure.restrict_apply_univ,smul_eq_mul,innerFieldVolume] using hb have hcoef : 0 ≤ 3*(packetDensityConstant/(h/4)^3)^2*innerFieldVolume h := by have := innerFieldVolume_nonneg h; positivity calc _ ≤ 3*(packetDensityConstant/(h/4)^3)^2*innerFieldVolume h*(innerFieldVolume h*F)+ 3*lam^2+3*(16*packetPotentialConstant)^2*T := add_le_add (add_le_add (mul_le_mul_of_nonneg_left hI hcoef) le_rfl) (mul_le_mul_of_nonneg_left ht (by positivity)) _ = _ := by ring end CoreObservationEnsemble end CoulombAtom end end OAI