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Add lean source and binary files (part 16)
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import Mathlib
import OAI.Analysis.CoulombIonization.Variational.CorePriceExcess
import OAI.Analysis.CoulombIonization.ThomasFermi.PatchTF
import OAI.Analysis.CoulombIonization.Variational.PatchMeasurable
namespace OAI
noncomputable section
namespace CoulombAtom
open MeasureTheory Filter
open scoped Topology BigOperators ContDiff
section Work_CoreFieldRegularity_scope
open MeasureTheory Filter Set Metric
open scoped BigOperators ContDiff
lemma coreCoulombAt_nonneg {N : ℕ} (ψ : FormVector N) (z : Space) :
0 ≤ coreCoulombAt ψ z := by
apply Finset.sum_nonneg
intro s _
apply Finset.sum_nonneg
intro i _
exact integral_nonneg (fun x => div_nonneg (sq_nonneg _) (norm_nonneg _))
lemma coreCoulombTerm_measurable {N : ℕ} {ψ : FormVector N} (hψ : SobolevVector ψ)
(s : Spins N) (i : Fin N) :
Measurable (fun z : Space => ∫ x, ‖ψ.value s x‖^2/‖x i-z‖) := by
let h := (hψ.1 s).aestronglyMeasurable
let v := h.mk (ψ.value s)
have hv : Measurable v := h.stronglyMeasurable_mk.measurable
have hm : StronglyMeasurable (fun q : Space × Configuration N => ‖v q.2‖^2/‖q.2 i-q.1‖) :=
(((hv.comp measurable_snd).norm.pow_const 2).div (by fun_prop)).stronglyMeasurable
have hh : Measurable (fun z : Space => ∫ x, ‖v x‖^2/‖x i-z‖) := hm.integral_prod_right.measurable
convert hh using 1
funext z
apply integral_congr_ae
filter_upwards [h.ae_eq_mk] with x hx
rw [hx]
lemma coreCoulombAt_measurable {N : ℕ} {ψ : FormVector N} (hψ : SobolevVector ψ) :
Measurable (coreCoulombAt ψ) :=
Finset.measurable_sum _ (fun s _ => Finset.measurable_sum _ (fun i _ => coreCoulombTerm_measurable hψ s i))
lemma normalizedCoreField_measurable {N : ℕ} {ψ : FormVector N} (hψ : SobolevVector ψ)
(Z lam : ℝ) : Measurable (normalizedCoreField Z lam ψ) :=
(((measurable_const.div continuous_norm.measurable).sub
(coreCoulombAt_measurable hψ)).div_const _).sub_const _
lemma coreCoulombTerm_le_separated {N : ℕ} {ψ : FormVector N} (hψ : SobolevVector ψ)
(A : Set Space) (hc : ∀ x i, x i ∉ A → FormZeroAt ψ x)
{d : ℝ} (hd : 0 < d) (z : Space) (hsep : ∀ a ∈ A, d ≤ ‖a-z‖)
(s : Spins N) (i : Fin N) :
(∫ x, ‖ψ.value s x‖^2/‖x i-z‖) ≤ (∫ x, ‖ψ.value s x‖^2)/d := by
rw [←integral_div]
apply integral_mono_of_nonneg
· exact Eventually.of_forall fun x => div_nonneg (sq_nonneg _) (norm_nonneg _)
· exact ((hψ.1 s).integrable_norm_pow (by decide)).div_const d
· apply Eventually.of_forall
intro x
dsimp only
by_cases hi : x i ∈ A
· exact div_le_div_of_nonneg_left (sq_nonneg _) hd (hsep _ hi)
· rw [(hc x i hi s).1]
simp only [norm_zero,zero_pow (by decide : (2:ℕ) ≠ 0),zero_div,le_refl]
lemma coreCoulombAt_le_separated {N : ℕ} {ψ : FormVector N} (hψ : SobolevVector ψ)
(A : Set Space) (hc : ∀ x i, x i ∉ A → FormZeroAt ψ x)
{d : ℝ} (hd : 0 < d) (z : Space) (hsep : ∀ a ∈ A, d ≤ ‖a-z‖) :
coreCoulombAt ψ z ≤ N*formMass ψ/d := by
have hh := Finset.sum_le_sum (s := Finset.univ) (fun s _ =>
Finset.sum_le_sum (s := Finset.univ) (fun i _ => coreCoulombTerm_le_separated hψ A hc hd z hsep s i))
simpa only [coreCoulombAt,Finset.sum_const,Finset.card_univ,Fintype.card_fin,nsmul_eq_mul, ←mul_div_assoc,←Finset.sum_div,←Finset.mul_sum,formMass] using hh
lemma normalizedCoreField_abs_le {N : ℕ} {ψ : FormVector N} (hψ : SobolevVector ψ)
(A : Set Space) (hc : ∀ x i, x i ∉ A → FormZeroAt ψ x)
{d : ℝ} (hd : 0 < d) (z : Space) (hsep : ∀ a ∈ A, d ≤ ‖a-z‖)
{r : ℝ} (hr : 0 < r) (hz : r ≤ ‖z‖) (Z lam : ℝ) :
|normalizedCoreField Z lam ψ z| ≤ |Z|/r+|lam|+N/d := by
by_cases hm : formMass ψ = 0
· simp only [normalizedCoreField,hm,mul_zero,zero_div,zero_sub,div_zero,abs_neg]
have : 0 ≤ (N:ℝ)/d := div_nonneg (Nat.cast_nonneg _) hd.le
have : 0 ≤ |Z|/r := div_nonneg (abs_nonneg _) hr.le
linarith
· have hmass : 0 < formMass ψ := lt_of_le_of_ne (formMass_nonneg ψ) (Ne.symm hm)
have hn := coreCoulombAt_nonneg ψ z
have hu := coreCoulombAt_le_separated hψ A hc hd z hsep
have he : normalizedCoreField Z lam ψ z = Z/‖z‖-coreCoulombAt ψ z/formMass ψ-lam := by
unfold normalizedCoreField
field_simp
rw [he]
have hab := abs_sub (Z/‖z‖-coreCoulombAt ψ z/formMass ψ) lam
have hab' := abs_sub (Z/‖z‖) (coreCoulombAt ψ z/formMass ψ)
have hZ : |Z/‖z‖| ≤ |Z|/r := by
rw [abs_div,abs_of_nonneg (norm_nonneg _)]
exact div_le_div_of_nonneg_left (abs_nonneg _) hr hz
have hc' : |coreCoulombAt ψ z/formMass ψ| ≤ N/d := by
rw [abs_of_nonneg (div_nonneg hn hmass.le)]
apply (div_le_iff₀ hmass).mpr
simpa only [mul_div_assoc, mul_comm (formMass ψ), div_mul_eq_mul_div] using hu
linarith
open CoulombAnalysis
lemma normalizedCoreField_memLp_patch {N : ℕ} {ψ : FormVector N} (hψ : SobolevVector ψ)
(A : Set Space) (hc : ∀ x i, x i ∉ A → FormZeroAt ψ x)
(y : Space) (R : ℝ) {d r : ℝ} (hd : 0 < d) (hr : 0 < r)
(hnuc : ∀ z ∈ closedBall y R, r ≤ ‖z‖)
(hsep : ∀ a ∈ A, ∀ z ∈ closedBall y R, d ≤ ‖a-z‖) (Z lam : ℝ) :
MemLp (fun x => normalizedCoreField Z lam ψ (y+x)) (5/2) (ballMeasure R) := by
apply MemLp.of_bound
(((normalizedCoreField_measurable hψ Z lam).comp (measurable_const.add measurable_id)).aestronglyMeasurable)
(|Z|/r+|lam|+N/d)
filter_upwards [ae_restrict_mem measurableSet_ball] with x hx
have hz : y+x ∈ closedBall y R := by
simpa only [mem_closedBall,dist_eq_norm,add_sub_cancel_left] using
(show ‖x‖ ≤ R from (by simpa only [mem_ball,dist_eq_norm,sub_zero] using hx : ‖x‖ < R).le)
rw [Real.norm_eq_abs]
exact normalizedCoreField_abs_le hψ A hc hd (y+x) (fun a ha => hsep a ha _ hz)
hr (hnuc _ hz) Z lam
end Work_CoreFieldRegularity_scope
open MeasureTheory Filter Set Metric
open scoped BigOperators ENNReal
open CoulombAnalysis
lemma coreSlice_field_measurable_rep {N M : ℕ} {ψ : FormVector (N+M)}
(hψ : SobolevVector ψ) (t : Spins M) (Z lam : ℝ) :
∃ F : Configuration M × Space → ℝ, Measurable F ∧
∀ᵐ u : Configuration M, ∀ z : Space,
F (u,z) = normalizedCoreField Z lam (coreSlice ψ t u) z := by
let d : Spins N → Configuration N × Configuration M → ℝ :=
fun s q => ‖ψ.value (joinLists s t) (joinLists q.1 q.2)‖^2
have hd (s : Spins N) : AEStronglyMeasurable (d s) :=
(integrable_join (N := N) (M := M) (hψ.1 (joinLists s t)).norm.integrable_sq).aestronglyMeasurable
let v : Spins N → Configuration N × Configuration M → ℝ := fun s => (hd s).mk (d s)
have hv (s : Spins N) : Measurable (v s) := (hd s).stronglyMeasurable_mk.measurable
have he (s : Spins N) : ∀ᵐ u : Configuration M, ∀ᵐ x : Configuration N,
d s (x,u) = v s (x,u) := by
have hh : d s =ᵐ[volume] v s := (hd s).ae_eq_mk
rw [Measure.volume_eq_prod] at hh
exact Measure.ae_ae_of_ae_prod (Measure.measurePreserving_swap.quasiMeasurePreserving.ae hh)
let m : Configuration M → ℝ := fun u => ∑ s : Spins N, ∫ x : Configuration N, v s (x,u)
have hm : Measurable m := by
apply Finset.measurable_sum
intro s _
exact (StronglyMeasurable.integral_prod_left (f := fun x u => v s (x,u))
(hv s).stronglyMeasurable).measurable
let V : Configuration M × Space → ℝ := fun q =>
∑ s : Spins N, ∑ i : Fin N, ∫ x : Configuration N, v s (x,q.1)/‖x i-q.2‖
have hV : Measurable V := by
apply Finset.measurable_sum
intro s _
apply Finset.measurable_sum
intro i _
have hh : Measurable (fun q : (Configuration M × Space) × Configuration N =>
v s (q.2,q.1.1)/‖q.2 i-q.1.2‖) :=
((hv s).comp (measurable_snd.prodMk (measurable_fst.fst))).div (by fun_prop)
exact hh.stronglyMeasurable.integral_prod_right.measurable
refine ⟨fun q => (Z*m q.1/‖q.2‖-V q)/m q.1-lam, ?_, ?_⟩
· exact (((measurable_const.mul (hm.comp measurable_fst)).div
(continuous_norm.measurable.comp measurable_snd)).sub hV).div
(hm.comp measurable_fst) |>.sub_const lam
· filter_upwards [ae_all_iff.mpr he] with u hu
have hm' : m u = formMass (coreSlice ψ t u) := by
apply Finset.sum_congr rfl
intro s _
apply integral_congr_ae
filter_upwards [hu s] with x hx
exact hx.symm
have hV' (z : Space) : V (u,z) = coreCoulombAt (coreSlice ψ t u) z := by
apply Finset.sum_congr rfl
intro s _
apply Finset.sum_congr rfl
intro i _
apply integral_congr_ae
filter_upwards [hu s] with x hx
exact congrArg (fun a : ℝ => a/‖x i-z‖) hx.symm
intro z
rw [hm',hV']
rfl
local instance : Fact ((5/2:ℝ≥0∞) ≠ ⊤) := ⟨by finiteness⟩
local instance (R : ℝ) : MeasurableSpace (TFField R) := borel _
local instance (R : ℝ) : BorelSpace (TFField R) := ⟨rfl⟩
local instance (R : ℝ) : MeasurableSpace (TFLp (ballMeasure R)) := borel _
local instance (R : ℝ) : BorelSpace (TFLp (ballMeasure R)) := ⟨rfl⟩
def conditionalPatchField {N M : ℕ} (ψ : FormVector (N+M)) (t : Spins M)
(Z lam : ℝ) (y : Space) (R : ℝ) (u : Configuration M) : TFField R :=
toLpOrZero (ballMeasure R) (5/2) (fun u z => normalizedCoreField Z lam (coreSlice ψ t u) (y+z)) u
lemma conditionalPatchField_aemeasurable {N M : ℕ} {ψ : FormVector (N+M)}
(hψ : SobolevVector ψ) (t : Spins M) (Z lam : ℝ) (y : Space) (R : ℝ) :
AEMeasurable (conditionalPatchField ψ t Z lam y R) := by
obtain ⟨F,hF,he⟩ := coreSlice_field_measurable_rep hψ t Z lam
have hm : Measurable (fun q : Configuration M × Space => F (q.1,y+q.2)) :=
hF.comp (measurable_fst.prodMk (measurable_const.add measurable_snd))
have hh := measurable_toLpOrZero (μ := ballMeasure R) (p := 5/2)
(f := fun u z => F (u,y+z)) hm
apply hh.aemeasurable.congr
filter_upwards [he] with u hu
apply toLpOrZero_congr (f := fun u z => F (u,y+z))
(g := fun u z => normalizedCoreField Z lam (coreSlice ψ t u) (y+z))
exact ae_of_all _ (fun z => hu (y+z))
lemma conditionalPatchMinimizer_aemeasurable {N M : ℕ} {ψ : FormVector (N+M)}
(hψ : SobolevVector ψ) (t : Spins M) (Z lam : ℝ) (y : Space) (R : ℝ) :
AEMeasurable (fun u => tfPatchMinimizer R tfKinetic tfKinetic_pos
(conditionalPatchField ψ t Z lam y R u)) :=
(tfPatchMinimizer_measurable R tfKinetic tfKinetic_pos).comp_aemeasurable
(conditionalPatchField_aemeasurable hψ t Z lam y R)
end CoulombAtom
end
end OAI