openAI-math-dataset / lean /OAI /Analysis /CoulombIonization /Fermionic /GlobalDensityConstant.lean
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Add lean source and binary files (part 16)
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import Mathlib
import OAI.Analysis.CoulombIonization.Fermionic.Density
import OAI.Analysis.CoulombIonization.Variational.Space
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
open MeasureTheory Set Metric
open scoped ENNReal
namespace CoulombAtom
namespace Pauli
open CoulombDensity
def globalDensityConstant : ℝ :=
192 + (8192/3:ℝ)*(8*Real.pi*(3/8192:ℝ)^(-3/2:ℝ)+3) + 8192/3
lemma globalDensityConstant_pos : 0 < globalDensityConstant := by
unfold globalDensityConstant
positivity
lemma density_nuclear_energy {N : ℕ} (ψ : FormVector (N+1)) (hψ : FormAdmissible ψ) (Z : ℝ) :
(∫ x, density ψ hψ.1 x*(Z/‖x‖)) =
Z*(∑ s : Spins (N+1), ∑ i : Fin (N+1),
∫ x : Configuration (N+1), ‖ψ.value s x‖^2/‖x i‖) := by
calc
_ = ∫ x, Z*(density ψ hψ.1 x/‖x‖) := by
apply integral_congr_ae
exact Filter.Eventually.of_forall (fun x => by ring)
_ = _ := by rw [integral_const_mul,(density_coulomb_integral ψ hψ).2]
theorem global_density_of_energy_le {N : ℕ} {Z δ : ℝ}
(hZ : 1 ≤ Z) (hδ : 0 ≤ δ) (hN : (N+1:ℝ) ≤ 3*Z)
(ψ : FormVector (N+1)) (hψ : FormAdmissible ψ) (he : formEnergy Z ψ ≤ δ) :
(∫ x, density ψ hψ.1 x^(5/3:ℝ)) ≤ globalDensityConstant * (Z^(7/3:ℝ)+δ) := by
let D := ∫ x, density ψ hψ.1 x^(5/3:ℝ)
let G := ∑ s : Spins (N+1), ∑ i : Fin (N+1), ∑ a : Fin 3,
∫ x : Configuration (N+1), ‖ψ.gradient s i a x‖^2
let A := ∑ s : Spins (N+1), ∑ i : Fin (N+1),
∫ x : Configuration (N+1), ‖ψ.value s x‖^2/‖x i‖
let B := 8*Real.pi*(3/8192:ℝ)^(-3/2:ℝ)+3
have hDp : 0 ≤ D := integral_nonneg (fun _ => Real.rpow_nonneg (density_nonneg _ _ _) _)
have hB : 0 ≤ B := by dsimp [B]; positivity
have hZp : 0 < Z := lt_of_lt_of_le zero_lt_one hZ
have hpow : Z ≤ Z^(7/3:ℝ) := by
calc
_ = Z^(1:ℝ) := (Real.rpow_one _).symm
_ ≤ _ := Real.rpow_le_rpow_of_exponent_le hZ (by norm_num)
have hp : 0 ≤ Z^(7/3:ℝ) := Real.rpow_nonneg hZp.le _
have hlt : D ≤ 32*(N+1:ℝ)+(2048/3:ℝ)*G := density_power_bound ψ hψ
have ha : Z*A ≤ (3/8192:ℝ)*D + B*Z^(7/3:ℝ) := by
have h := nuclear_density_scaled (density ψ hψ.1) (density_nonneg ψ hψ.1)
(density_integrable ψ hψ.1) (density_power_integrable ψ hψ) hZp
(by norm_num : (0:ℝ) < 3/8192) (by rw [density_mass ψ hψ]; exact hN)
rwa [density_nuclear_energy ψ hψ Z] at h
have hr : 0 ≤ (∑ s : Spins (N+1), ∑ i : Fin (N+1), ∑ j : Fin (N+1),
if i < j then (∫ x : Configuration (N+1), ‖ψ.value s x‖^2/‖x i-x j‖) else 0) := by
apply Finset.sum_nonneg
intro s _
apply Finset.sum_nonneg
intro i _
apply Finset.sum_nonneg
intro j _
split_ifs <;> positivity
have hkin : (1/2:ℝ)*G - Z*A ≤ δ := by
dsimp [formEnergy] at he
dsimp [G,A]
linarith
have hbase : D ≤ (192+(8192/3:ℝ)*B)*Z^(7/3:ℝ)+(8192/3:ℝ)*δ := by
nlinarith
have hc : globalDensityConstant = 192+(8192/3:ℝ)*B+8192/3 := rfl
rw [hc]
nlinarith
end Pauli
end CoulombAtom
end
end OAI