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LeanPool.Superdiffusion.Algsuperdiff.Section4.Provider.ExcessDecay.ResidueAbsorption

ResidueAbsorption #

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

The residue routes, measured: three machine-checked obstructions #

This module records, as theorems, the exact inequalities that block the two candidate producers for the harmonic-approximation residue ‖u − w‖_{L²(K')} of ResidueBudget, with K' = flushSubCentre z m n i σ + □_n the flush scale-n sub-cube of the boundary branch and w a Δ-harmonic comparator of u there. Nothing here is an analytic estimate; each theorem is the arithmetic or geometric core of one measured route, isolated so that the STOP table is checked rather than asserted.

So a residue producer may output exactly

  ‖u − w‖_{L²(K')} ≤ K1 · ‖u − (u)_{W'}‖_{L²(W')}
                    + K2 · 3^n ‖∇h‖_{L²(W')}
                    + K3 · s^{-2} 3^{(1+s)n} [∇h]_{H^s(W')}
                    + K4 · s^{-3} σ_n^{-1} 3^{(1+s)n} [g]_{H^s(W')}

with K1..K4 constants: the four allowed s-powers are 0, 0, −2, −3 and only the last carries a σ^{-1}. Both routes below fail against this contract, each by one uniform factor.

Route 1 — the p = 2 coarse-graining comparison at K' #

The proved interior chain (InteriorEllipticitySlot.eLpNorm_sub_weaklyHarmonic_le_coarseGraining_rebased composed with AssemblyEnergyLeg.ae_h1EnergyNormOnCube_boundary_le_anchorLegs) prices a comparator distance in the shape

  ‖u − w‖ ≤ A · s^{-4} · 𝓔 · ( ‖u − (u)_{W'}‖ + S ) + (s^{-6}, s^{-7}σ^{-1} legs) ,

so the budget's first-leg coefficient would be K1 = A·s^{-4}·𝓔, not a constant. coarseGrainingResidue_coefficient_unbounded is the refutation: for any fixed error level E > 0 — in particular for the level the frozen good event pins, 𝓔 ≤ C_E·ε at ε = 1/2 — and any candidate constant, some admissible s ∈ (0,1] exceeds it. coarseGrainingResidue_loop_not_contraction is the same statement read as the self-consistency loop S ≤ a + θ·S: the loop coefficient θ = A·s^{-4}·𝓔 is not below 1 uniformly, so the residue cannot be solved for either. Closing the route needs 𝓔 ≲ s^4, i.e. the good event's ε re-pinned at c·s^4 — a change to the frozen statement.

Route 1′/option (ii) — the fitted boundary Caccioppoli at K' #

SealCaccioppoliGeometry.flushSubCube_boundaryOuterAssembly_fits prices the ν-weighted energy ν·⨍_{K'}|∇u|² against a coarse-grained Λ_t-weighted right-hand side, so extracting a ν-free comparator distance costs √(Λ_t/ν) ≤ C√(σ/ν). energyRatio_sqrt_unbounded records that no constant absorbs √(σ/ν) over 0 < ν ≤ σ. (That the ratio really is unbounded on the model family is ABK26's Theorem A; it is cited, not proved here.)

Route 2 — the anchor's own good event at the sub-scale #

Every proved transfer that would put an error cap, an ellipticity cap, or the anchor's own conclusion on a scale-n cube requires the anchor's geometry binder x + □_n ⊆ (z+□_{n+1}) ∩ □_m — see InteriorGlueCap.ae_offGridChildError_le_representative_harmonicSlot and AssemblyEnergyLeg.ae_h1EnergyNormOnCube_boundary_le_anchorLegs. exists_flushSubCube_not_subset_anchorGeometry exhibits an admissible boundary-branch configuration in which K' satisfies K' ⊆ □_m but not K' ⊆ z + □_{n+1}: the flush sub-cube is pushed 4·3^n off z while z + □_{n+1} reaches only 3^n. And no_flushCentre_within_anchorGeometry shows this is intrinsic, not a bad choice of K': on the whole sub-range ½·3^m − 9/2·3^n < σ·zᵢ < ½·3^m − 3/2·3^n of the boundary branch (nonempty by wellPlacedHalfGap_lt_farThreshold, width 3·3^n) no flush scale-n centre satisfies the binder. So the caps are not available at K' as proved, independently of the arithmetic above.

The scope of that obstruction: it is a statement about the proved binders, not a proof that the underlying apparatus cannot be re-instantiated. InteriorGlueCap.ae_offGridChildError_le_representative_translate is already stated for an arbitrary real translate with w + □_n ⊆ □_{n+2}, and K' does satisfy the corresponding gap-three containment c' − z + □_n ⊆ □_{n+3} at the frozen (n+3, z) frame; re-cutting that cap and the ellipticity caps at the (n+3) parent is bounded provider work. The arithmetic obstruction of Route 1 is the one that does not move.

References #

1. Route 1: the s^{-4}·𝓔 coefficient is not a constant #

The display's s^{-4} written as a natural power of s⁻¹.

theorem Algsuperdiff.Section4.Provider.ExcessDecay.coarseGrainingResidue_coefficient_le_of_error_small {A E s : ℝ} (hs : 0 < s) (hA : 0 ≤ A) (hE : 0 ≤ E) (hsmall : A * E ≤ s ^ 4) :
A * s.rpow (-4) * E ≤ 1

The exact closing condition for route 1.

If the error level obeys A·E ≤ s^4 then — and, by coarseGrainingResidue_coefficient_unbounded, essentially only then — the coefficient is bounded by 1. This is the ε ≤ c·s^4 re-pinning of the good event: a change to the frozen statement.

2. Route 1′ / option (ii): the √(σ/ν) cost is not absorbable #

3. Route 2: the anchor's geometry binder fails at the flush sub-cube #