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Add lean source and binary files (part 16)
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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