ResidueRouteOne #
Ported from scottnarmstrong/Superdiffusion at 7f20476385d4af418f110303085ad0740c9eba46. Module imports, support namespace and local option directives adapted for Lean Pool.
Route 1, machine-assembled at the flush sub-cube K' #
Nothing here imports that file, and nothing here claims the anchor or any source node.
What is proved #
derived, from the shapes of the proved theorems, that the p = 2
coarse-graining comparison read at the flush scale-n sub-cube K' = flushSubCentre z m n i σ + □_n prices the harmonic-approximation residue ‖u − w‖_{L²(K')} on the five canonical legs, but could not assemble it, because
the proved caps carry the anchor's geometry binder and K' provably fails it.
This module is that assembly:
‖u − w‖_{L²(K')} ≤ Cfin ·
( s^{-4}·𝓔·‖u − (u)_{W'}‖_{L²(W')}
+ s^{-7}·σ_{n+3}^{-1}·3^{(1+s)n}·[g]_{H^s(W')}
+ s^{-6}·3^{(1+s)n}·[∇h]_{H^s(W')}
+ s^{-6}·3^{n}·‖∇h‖_{L²(W')}
+ s^{-4}·𝓔·S )
with 𝓔 = fluxCorrectedErrorRepresentative M L (n+3) ⟨s/8⟩ (translate z ω)
carried explicitly (not substituted by the frozen good event's ε = 1/2),
and S the boundary scalar at the flush cube K = wellPlacedCentre z m (n+2) + □_{n+2} — which is the covering cube of K'
(ResidueCapGeometry.wellPlacedCentre_flushSubCentre).
- the deterministic
x-frame envelopeReindexEllipticity.eLpNorm_sub_weaklyHarmonic_le_coarseGraining_rebased_addThree(binder-free: it needs onlytranslateSet x □_n ⊆ □_m); - the boundary energy leg at the two hinges (
ResidueEnergyLeg); - the child cube's
𝓔-cap and forcing bracket at hinge (C) (ResidueCapChild); - the one-hop Gagliardo transport
K' → W'(ResidueFlushTransport) in place of the proved two-hop route through the(n+2)window, whichK'does not meet.
The σ-cancellation, machine-verified #
The envelope is divided by σ₀ = σ_{n+3} and the energy term carries
‖a₀‖^{1/2} = √σ_{n+3} (constantCoeffMatrixNormHalf_scalarComparator_sqrt).
The two identities √σ·√σ = σ and √σ·√(σ^{-1}) = 1 are consumed at h1 and h2
below: they cancel σ exactly on the four √σ legs and leave exactly one
σ^{-1} on the force leg. No ν is divided anywhere: CoarseGraining's
h1EnergyNormOnCube at the re-based family equals √(ν·⨍|∇u|²), and that
quantity is consumed whole by the boundary energy leg — it is never converted
to a Euclidean gradient.
References #
- ABK26,
l.harmonic.approximation.good.scales; the boundary application;e.homogenization.L2.interior.
Child-cube geometry and transport facts shared by the two boundary routes.
Equations
- One or more equations did not get rendered due to their size.
Instances For
The energy comparison contract shared by the two boundary routes.
Equations
- One or more equations did not get rendered due to their size.
Instances For
Route 1, composed at the flush sub-cube — the error-weighted legs.
The harmonic-approximation residue at K', priced on the five canonical legs
with the good-event error 𝓔 carried explicitly. As in AssemblyComposedErrorWeighted,
the monotone discard is declined on the flat ∇h row, so that leg reads
s^{-6}·𝓔·3^n·‖∇h‖_{L²(W')}.