The comparison density rhoA a (the proof notes (8′), (11′), (15′)).
rhoA a = ∫ g(c) ρ_c dc (CIntegrals); Tonelli/Fubini in (t, c) turns ∫ φ · rhoA into ∫ g(c) ∫ φ · ρ_c.
With the per-component potentials (Poisson) and the g-integrals of kC, wC this gives
2L − W = ℓ on [-a, a], 2L − W ≤ ℓ everywhere, and 2I − W = ℓ, ℓ = ellA a, when
massA a = 1.
theorem
Zeta32.Analytic.EnergyI.measurable_rhoC
(a : ℝ)
:
Measurable fun (p : ℝ × ℝ) => rhoC a p.2 p.1
theorem
Zeta32.Analytic.EnergyI.fubini_rhoA
{a : ℝ}
(ha : 0 < a)
(φ : ℝ → ℝ)
(hφm : Measurable φ)
(hφ : IntervalIntegrable (fun (t : ℝ) => |φ t| * rhoA a t) MeasureTheory.volume (-a) a)
:
theorem
Zeta32.Analytic.EnergyI.rhoA_good
{a : ℝ}
(ha : 0 < a)
(hm : massA a = 1)
:
GoodDensity (rhoA a) a
theorem
Zeta32.Analytic.EnergyI.intervalIntegrable_Wt_abs_rhoA
{a : ℝ}
(ha : 0 < a)
:
IntervalIntegrable (fun (x : ℝ) => Wt |x| * rhoA a x) MeasureTheory.volume 0 a