File size: 11,182 Bytes
159357f | 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60 61 62 63 64 65 66 67 68 69 70 71 72 73 74 75 76 77 78 79 80 81 82 83 84 85 86 87 88 89 90 91 92 93 94 95 96 97 98 99 100 101 102 103 104 105 106 107 108 109 110 111 112 113 114 115 116 117 118 119 120 121 122 123 124 125 126 127 128 129 130 131 132 133 134 135 136 137 138 139 140 141 142 143 144 145 146 147 148 149 150 151 152 153 154 155 156 157 158 159 160 161 162 163 164 165 166 167 168 169 170 171 172 173 174 175 176 177 178 179 180 181 182 183 184 185 186 187 188 189 190 191 192 193 194 195 196 197 198 199 200 201 202 203 204 205 206 207 208 209 210 211 212 213 | import Mathlib
import OAI.Analysis.CoulombIonization.Ionization.PricedCoulombTail
import OAI.Analysis.CoulombIonization.FieldAnalysis.ObservedFieldScale
namespace OAI
noncomputable section
namespace CoulombAtom
section
open MeasureTheory Set
lemma annular_cut_cost_innerScale {D h u : ℝ} (hD : 0 ≤ D) (hh : 0 < h) (hu : h ≤ u) :
(annularOffsetMass D u)^2/u/h ≤ 3*innerScale D h := by
have hup : 0 < u := hh.trans_le hu
calc
_ ≤ (3*(1/u^6+1+D*u))/u/h :=
div_le_div_of_nonneg_right (div_le_div_of_nonneg_right (annularOffsetMass_sq_le hD hup) hup.le) hh.le
_ = 3*((1/u^7)/h+(1/u)/h+D/h) := by field_simp
_ ≤ 3*((1/h^7)/h+(1/h)/h+D/h) := by gcongr
_ = _ := by unfold innerScale; field_simp
lemma finite_annular_excess_at_innerScale {N : ℕ} {psi : FormVector N}
(hpsi : SobolevFermion psi) (hm : formMass psi = 1) {Z lam alpha beta u D h : ℝ}
(hZ : 0 ≤ Z) (hlam : 0 < lam) (ha : 0 < alpha) (hD : 0 ≤ D) (hh : 0 < h) (hu : h ≤ u)
(he : max (corePriceExcess Z lam psi) 0 ≤ D) (ys : List Space)
(hys : ∀ y ∈ ys, alpha*u ≤ ‖y‖ ∧ ‖y‖ ≤ beta*u) :
max (((CoreObservationEnsemble.initial psi hpsi).observeCells ys).excess Z lam) 0/h ≤
((radialCutExcessConstant actualCellMomentConstant+1)^ys.length*
(1+3*annularCellCostConstant alpha beta))*innerScale D h := by
have hbase := actual_finite_annular_cut_excess hpsi hm hZ hlam ha (hh.trans_le hu) hD he ys hys
have hcost := annular_cut_cost_innerScale hD hh hu
have hC := (annularCellCostConstant_pos (beta := beta) ha).le
have hK : 0 ≤ (radialCutExcessConstant actualCellMomentConstant+1)^ys.length := by
have := radialCutExcessConstant_one_le actualCellMomentConstant_one_le
positivity
have hD' : D/h ≤ innerScale D h := by
unfold innerScale
have h1 : 0 ≤ 1/h^8 := by positivity
have h2 : 0 ≤ 1/h^2 := by positivity
linarith
calc
_ ≤ ((radialCutExcessConstant actualCellMomentConstant+1)^ys.length*
(D+annularCellCostConstant alpha beta*(annularOffsetMass D u)^2/u))/h :=
div_le_div_of_nonneg_right hbase hh.le
_ = (radialCutExcessConstant actualCellMomentConstant+1)^ys.length*
(D/h+annularCellCostConstant alpha beta*((annularOffsetMass D u)^2/u/h)) := by ring
_ ≤ (radialCutExcessConstant actualCellMomentConstant+1)^ys.length*
(innerScale D h+annularCellCostConstant alpha beta*(3*innerScale D h)) :=
mul_le_mul_of_nonneg_left (add_le_add hD' (mul_le_mul_of_nonneg_left hcost hC)) hK
_ = _ := by ring
lemma actual_observed_local_count {N : ℕ} {psi : FormVector N}
(hpsi : SobolevFermion psi) (hm : formMass psi = 1) {Z lam D : ℝ}
(hZ : 0 ≤ Z) (hlam : 0 < lam) (he : max (corePriceExcess Z lam psi) 0 ≤ D)
(ys : List Space) {z : Space} (hz : z ≠ 0) :
((CoreObservationEnsemble.initial psi hpsi).observeCells ys).countMoment z (8*localCellRadius z) ≤
actualCellMomentConstant*(localOffsetMass D z)^2 := by
let E := CoreObservationEnsemble.initial psi hpsi
have hr := localCellRadius_pos hz
calc
_ ≤ E.countMoment z (8*localCellRadius z) := E.observeCells_countMoment ys _ _
_ ≤ E.countMoment z (32*localCellRadius z) := E.countMoment_le_of_radius z z
(by simp only [sub_self,norm_zero,zero_add]; linarith)
_ = rawCountMoment psi z (32*localCellRadius z) := CoreObservationEnsemble.initial_countMoment ..
_ ≤ actualCellMomentConstant*(localOffsetMass (max (corePriceExcess Z lam psi) 0) z)^2 :=
priced_enlarged_cell_count hpsi hm hZ hlam hz
_ ≤ _ := mul_le_mul_of_nonneg_left (pow_le_pow_left₀
(zero_le_one.trans (localOffsetMass_one_le _ z)) (localOffsetMass_mono he z) 2)
(zero_le_one.trans actualCellMomentConstant_one_le)
theorem exists_actual_observed_innerCap_constant {alpha beta : ℝ} (ha : 0 < alpha) (L : ℕ) :
∃ C : ℝ, 1 ≤ C ∧ ∀ (Z lam : ℝ) (N : ℕ) (psi : FormVector N) (hpsi : SobolevFermion psi),
formMass psi = 1 → 0 ≤ Z → 0 < lam → ∀ (D h u : ℝ), 0 ≤ D → 0 < h → h ≤ u →
max (corePriceExcess Z lam psi) 0 ≤ D → ∀ ys : List Space, ys.length = L →
(∀ y ∈ ys, alpha*u ≤ ‖y‖ ∧ ‖y‖ ≤ beta*u) →
((CoreObservationEnsemble.initial psi hpsi).observeCells ys).innerCapAverage Z lam h ≤
C*(innerScale D h+lam^2) := by
obtain ⟨T,hT,hTail⟩ := exists_priced_coulomb_tail_constant
let A := (radialCutExcessConstant actualCellMomentConstant+1)^L*(1+3*annularCellCostConstant alpha beta)
let F := localFieldUniversalConstant*(100000*A+(5+actualCellMomentConstant)*3*(annularCellScaleConstant 1 3*100000)^2)
let K := 3*(packetDensityConstant*64*(36*Real.pi))^2*F+3*(16*packetPotentialConstant)^2*T
let C := max K 3
have hA : 0 ≤ A := by
have := radialCutExcessConstant_one_le actualCellMomentConstant_one_le
have := annularCellCostConstant_pos (beta := beta) ha
dsimp [A]; positivity
have hF : 0 ≤ F := by
have := localFieldUniversalConstant_pos
have := actualCellMomentConstant_one_le
dsimp [F]; positivity
refine ⟨C,(by dsimp [C]; exact (by norm_num : (1:ℝ) ≤ 3).trans (le_max_right _ _)),?_⟩
intro Z lam N psi hpsi hm hZ hlam D h u hD hh hu he ys hlen hys
let E := (CoreObservationEnsemble.initial psi hpsi).observeCells ys
have hmE : E.mass = 1 := (CoreObservationEnsemble.observeCells_mass ..).trans ((CoreObservationEnsemble.initial_mass ..).trans hm)
have hEx : max (E.excess Z lam) 0/h ≤ A*innerScale D h := by
simpa only [E,A,hlen] using finite_annular_excess_at_innerScale hpsi hm hZ hlam ha hD hh hu he ys hys
have hf : ∀ z ∈ innerFieldTestAnnulus h, E.fieldMoment Z lam z ≤ F*innerScale D h := by
intro z hz
exact ensemble_field_annular_bound E hZ hlam hD hh hmE hEx
(fun z hz => actual_observed_local_count hpsi hm hZ hlam he ys (norm_pos_iff.mp (hh.trans_le hz.1))) hz
have ht : E.weightedMoment (coulombTailWeight h) ≤ T*innerScale D h := by
calc
_ ≤ (CoreObservationEnsemble.initial psi hpsi).weightedMoment (coulombTailWeight h) :=
CoreObservationEnsemble.observeCells_weightedMoment _ ys (coulombTailWeight_measurable h)
(coulombTailWeight_nonneg h) (coulombTailWeight_le hh)
_ = rawWeightedMoment psi (coulombTailWeight h) := CoreObservationEnsemble.initial_weightedMoment ..
_ ≤ _ := hTail Z lam N psi hpsi hm hZ hlam D h hD hh he
have hb := innerCapAverage_scale E hZ hlam.le hD hh hmE hF hf ht
calc
_ ≤ K*innerScale D h+3*lam^2 := hb
_ ≤ C*innerScale D h+C*lam^2 := add_le_add
(mul_le_mul_of_nonneg_right (le_max_left _ _) (innerScale_nonneg hD hh))
(mul_le_mul_of_nonneg_right (le_max_right _ _) (sq_nonneg _))
_ = _ := by ring
end
open MeasureTheory Filter
open scoped BigOperators
structure FullStatistic where
value : ∀ N, Configuration N → ℝ
measurable : ∀ N, Measurable (value N)
bounded : ∀ N, ∃ B : ℝ, ∀ x, ‖value N x‖ ≤ B
reindex : ∀ {M N} (e : Fin M ≃ Fin N) (x : Configuration M),
value N (x ∘ e.symm) = value M x
lemma rawFormPair_reindex {M N : ℕ} (e : Fin M ≃ Fin N) (psi : FormVector N)
(F : FullStatistic) : rawFormPair (reindexForm e psi) (F.value M) = rawFormPair psi (F.value N) := by
have he (s : Spins M) :
(∫ x, F.value M x*‖(reindexForm e psi).value s x‖^2) =
∫ x, F.value N x*‖psi.value (s ∘ e.symm) x‖^2 := by
simpa only [reindexForm,F.reindex] using
integral_reindex e (fun x => F.value N x*‖psi.value (s ∘ e.symm) x‖^2)
unfold rawFormPair
simp_rw [he]
exact sum_spin_reindex e (fun s : Spins N => ∫ x, F.value N x*‖psi.value s x‖^2)
lemma rawFormPair_nextCoreObservation {N M : ℕ}
(p : Fin 2 → SmoothMultiplier spaceDirections) (hp : ∀ x, ∑ a, (p a).value x^2=1)
(psi : FormVector (N+M)) (c : Fin N → Fin 2) (F : FullStatistic) :
rawFormPair (nextCoreObservation p hp psi c) (F.value _) =
rawFormPair (multiplyForm (coreLiftMultiplier M (spatialProduct p hp c)) psi) (F.value _) := by
unfold nextCoreObservation repeatedCutForm
rw [rawFormPair_reindex,rawFormPair_reindex]
lemma sum_rawFormPair_nextCoreObservation {N M : ℕ} {psi : FormVector (N+M)}
(hpsi : SobolevVector psi) (p : Fin 2 → SmoothMultiplier spaceDirections)
(hp : ∀ x, ∑ a, (p a).value x^2=1) (F : FullStatistic) :
(∑ c : Fin N → Fin 2, rawFormPair (nextCoreObservation p hp psi c) (F.value _)) =
rawFormPair psi (F.value _) := by
simp_rw [rawFormPair_nextCoreObservation]
obtain ⟨B,hB⟩ := F.bounded (N+M)
unfold rawFormPair
rw [Finset.sum_comm]
apply Finset.sum_congr rfl
intro s _
have hi (c : Fin N → Fin 2) : Integrable (fun x => F.value (N+M) x*
‖(multiplyForm (coreLiftMultiplier M (spatialProduct p hp c)) psi).value s x‖^2) :=
(((hpsi.multiply _).1 s).norm.integrable_sq).bdd_mul (F.measurable _).aestronglyMeasurable
(ae_of_all _ hB)
rw [←integral_finsetSum _ (fun c _ => hi c)]
apply integral_congr_ae
apply ae_of_all
intro x
have hs : ∑ c : Fin N → Fin 2, (coreLiftMultiplier M (spatialProduct p hp c)).value x^2 = 1 := by
exact spatial_square_partition p hp (leftList x)
simp only [multiplyForm,Complex.norm_mul,Complex.norm_real,Real.norm_eq_abs,mul_pow,sq_abs]
rw [←Finset.mul_sum,←Finset.sum_mul,hs]
ring
namespace CoreObservationGraph
def fullAverage (G : CoreObservationGraph) (F : FullStatistic) : ℝ :=
rawFormPair G.vector (F.value _)
lemma observe_fullAverage (G : CoreObservationGraph)
(p : Fin 2 → SmoothMultiplier spaceDirections) (hp : ∀ x, ∑ a, (p a).value x^2=1)
(F : FullStatistic) :
(∑ c : Fin G.coreSize → Fin 2, (G.observe p hp c).fullAverage F) = G.fullAverage F :=
sum_rawFormPair_nextCoreObservation G.sobolev p hp F
end CoreObservationGraph
namespace CoreObservationEnsemble
def fullAverage (E : CoreObservationEnsemble) (F : FullStatistic) : ℝ :=
∑ i, (E.graph i).fullAverage F
lemma initial_fullAverage {N : ℕ} (psi : FormVector N) (hpsi : SobolevFermion psi) (F : FullStatistic) :
(initial psi hpsi).fullAverage F = rawFormPair psi (F.value N) := by
change (∑ _i : Unit, rawFormPair psi (F.value N)) = _
simp
lemma observe_fullAverage (E : CoreObservationEnsemble)
(p : Fin 2 → SmoothMultiplier spaceDirections) (hp : ∀ x, ∑ a, (p a).value x^2=1)
(F : FullStatistic) : (E.observe p hp).fullAverage F = E.fullAverage F := by
change (∑ ic : Σ i : E.Branch, Fin (E.graph i).coreSize → Fin 2,
((E.graph ic.1).observe p hp ic.2).fullAverage F) = _
rw [Fintype.sum_sigma]
exact Finset.sum_congr rfl (fun i _ => (E.graph i).observe_fullAverage p hp F)
lemma observeCells_fullAverage (E : CoreObservationEnsemble) (ys : List Space) (F : FullStatistic) :
(E.observeCells ys).fullAverage F = E.fullAverage F := by
induction ys generalizing E with
| nil => rfl
| cons y ys ih =>
rw [observeCells,ih]
unfold observeCell
split_ifs
· rfl
· exact observe_fullAverage E _ _ F
end CoreObservationEnsemble
end CoulombAtom
end
end OAI
|