HomSchauderUniform #
Ported from scottnarmstrong/Superdiffusion at 7f20476385d4af418f110303085ad0740c9eba46. Module imports, support namespace and local option directives adapted for Lean Pool.
The s-UNIFORM Schauder constant, and the K_abs frame condition it closes #
The trap #
The §4.5 Step-4 Schauder constant C_S4(d,s) is a Classical.choose of an
s-indexed existential. Its defining property is UPWARD CLOSED in the
constant, so nothing in the tree bounds the chosen value: the frame condition
spineClauseConst d s p C_w (C_S4 d s) ≤ K_abs
can be met at each fixed s, but NOT by one K_abs produced before the model
— and at the §4.5 pin s = |log γ|⁻¹ the exponent is a function of the model.
That is a genuine obstruction to Theorem B's constant scope, not a bookkeeping
nuisance.
The s = 1/2 reduction #
The underlying producer's constant does not depend on s at all
(Section4.Provider.Schauder.cube_schauder_of_zeroDatumCubeSchauder returns
2·C₀ + 1 with C₀ the zero-datum constant), and the s-package is in any
case a consequence of the s = 1/2 package on a triadic cube: on □_m the two
points of a Hölder difference are at distance at most 3^m, so
[f]_{C^{0,s}(□_m)} ≤ 3^{m(1/2 - s)} [f]_{C^{0,1/2}(□_m)},
and the target's own weight 3^{-sm} absorbs the factor EXACTLY: multiplying
the s = 1/2 gauge estimate by 3^{m(1/2-s)} turns
3^{-m/2}K_sup + K_Höl ≤ C 3^{-m/2} ⟨data⟩ into
3^{-sm}K_sup + 3^{m(1/2-s)}K_Höl ≤ C 3^{-sm} ⟨data⟩, with the SAME C.
exists_comparator_schauder_package_uniform is that statement, and
stepFourSchauderConstU d is its s-free constant. spineClauseConst_le_abs
then closes the frame condition at a K_abs naming only d and an envelope
for C_w — both available before the model.
Scope #
The §4.5 bundle core refers to C_S4(d, s.1) inside its hKabs conjunct, so
consuming the uniform constant requires a SIBLING of that bundle (and of the
re-cut's two consumption sites, which spend hKabs through spineClauseConst)
with C_S4(d, s.1) replaced by stepFourSchauderConstU d. That re-cut is NOT performed here;
what is proved here is that the replacement is sound — the uniform constant
satisfies the same package at every admissible s.
1. The Hölder order step #
The Hölder order step on a bounded set. Lowering the exponent from
α to β ≤ α costs exactly the (α-β)-th power of the diameter.
2. The s-uniform package #
THE s-UNIFORM SCHAUDER PACKAGE.
One constant, produced before the exponent s, the scale m, the diffusivity
and the data, serving the whole admissible range 0 < s ≤ 1/2: the comparator
of HomStepFourSchauder.exists_comparator_schauder_package at the SAME
constant for every s.
The proof runs the s = 1/2 package once and lowers the Hölder exponent on
□_m; the loss 3^{m(1/2-s)} is exactly cancelled by the gauge's own
3^{-sm}, so no constant is spent.
3. The s-free constant and the K_abs closure #
THE s-UNIFORM SCHAUDER CONSTANT. Unlike the s-indexed Step-4
Schauder constant, this is a Classical.choose of an s-FREE existential, so it
is a function of d alone.
Equations
- Algsuperdiff.Section4.Provider.Homogenization.stepFourSchauderConstU d = if h : 2 ≤ d then Classical.choose ⋯ else 0
Instances For
THE K_abs FRAME CONDITION, CLOSED BEFORE THE MODEL.
At the uniform Schauder constant, the absorbed-constant condition of the re-cut bundle holds at
K_abs:= (2 · stepFourSchauderConstU d + 288 d²) · C_w⁰,
which names only the dimension and an envelope C_w⁰ for the pairing constant
— no s, hence no model. The only s-dependence of spineClauseConst is the
lifting factor liftGeomFactor (s + d/p), and the bundle's OWN guard
s + d/p ≤ 1/2 bounds it by 3.