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LeanPool.Superdiffusion.Algsuperdiff.Section4.Provider.Homogenization.HomFinitePConversion

HomFinitePConversion #

Ported from scottnarmstrong/Superdiffusion at 7f20476385d4af418f110303085ad0740c9eba46. Module imports, support namespace and local option directives adapted for Lean Pool.

Theorem B, §4.5, Step 3c: the finite-p conversion #

THE CONVERSION #

The L^∞ endpoint is taken from the PRINTED finite-p proposition rather than from its p ↑ ∞ limit. The mechanism is an exponent shift, and the conversion is a four-step chain, every step proved:

  (1)  3^{-ms}‖∇u-∇v‖_{B^{-s}_{p,p}(□_m)} ≤ A          (hCG', printed carrier)
  (2)  ⟹  |(∇u-∇v)_R| ≤ A·3^{(s+d/p)·depth R}          (HomFinitePGauge: one term
                                                        out of 3^{jd}, constant 1)
  (3)  ⟹  ‖(∇u-∇v)_{x+□_n}‖ ≤ 6dγ·A·3^{(s+d/p)(m-n)}   (HomFinitePTranslate:
                                                        the Whitney tiling, γ = liftGeomFactor)
  (4)  ⟹  3^{-m}|u-v| ≤ 16d·6dγ·A = 96 d² γ A a.e.     (the endpoint)

The 3^{m(s+d/p)} prefactor cancels exactly. Step (2) produces the gauge constant A·3^{m s'} at the shifted order s' = s + d/p, and the endpoint multiplies by 3^{-m s'} (linfty_constant_cancels). So the finite-p route gives on the SAME display as the (∞,∞) route with L replaced by the finite-p gauge level, at the dimension-only constant 96 d² γ (≤ 288 d² at the Step-3 pin, since γ = liftGeomFactor s' ≤ 3).

THE RANGE GUARD, and where it is discharged #

The chain requires 0 < s' ≤ 1/2, i.e. s + d/p ≤ 1/2. At the author's p = 4d this is d/p = 1/4, hence exactly s ≤ 1/4 — which is the Step-3 pin already in force: s = |log γ|^{-1} with the homS_le_quarter at 4 ≤ |log γ|. The guard is an explicit hypothesis at every statement (hguard), never silent.

Carriers: no harvest, no deviation #

hCG' is stated at the PRINTED grid-summed carrier (the negative Besov seminorm definition's pure lattice 3^k ℤ^d ∩ □_m = CoarseGraining's descendantsAtDepth). The grid/translate carrier mismatch is DISCHARGED here by HomFinitePTranslate.uniformBoxGaugeBound_of_gridGauge: the reconstruction is proved. The only extra frame item it needs is that the field vanishes off □_m, which is the H¹₀ zero extension already present in the frame.

Main results #

Steps (2)–(4) are carried at the print's own sup-over-depths gauge, in HomSpineSupFormRethread.

1. The cancellation and the guard, displayed #

theorem Algsuperdiff.Section4.Provider.Homogenization.linfty_constant_cancels (m : ℤ) (K A s' : ℝ) :
K * (A * 3 ^ (s' * ↑m)) * 3 ^ (-↑m * s') = K * A

THE 3^{m(s+d/p)} CANCELLATION.

The extraction inflates the gauge constant by 3^{m s'} and the endpoint deflates it by 3^{-m s'}; the two are inverse. Nothing about p survives into the L^∞ display except through the exponent guard.