MomentHolder #
Ported from scottnarmstrong/Superdiffusion at 7f20476385d4af418f110303085ad0740c9eba46. Module imports, support namespace and local option directives adapted for Lean Pool.
Step 5's Hölder bookkeeping, in the anchor's lintegral normal form #
What this module supplies #
Step 5 of the proof of l.bounds.mathcal.E.aL reads:
Using these estimates, the restrictions
m − n ≤ γ^{-1}andp ≤ C^{-1}γ^{-1}sand Hölder's inequality, it is straightforward to see that thep-th root of the sum overj ≤ nof thep/2-th moment of the first and third terms ... is bounded by the right side.
Each term of e.apply.sensitivity.J.aL is a PRODUCT of the Step-4 bullets, and
each bullet is available at EVERY moment q ∈ [1,∞) (that is exactly what the
hence, for every q sentences of Step 4 deliver).
Hölder therefore costs nothing except a uniform boost of the exponent by the
number of factors.
lintegral_rpow_prod_le_of_moments— anN-factor product whose factors each obey the normal form at the boosted exponentN qobeys it atq, with the product of the majorants. This is the reconstruction of the source's "Hölder's inequality" for the four terms.lintegral_rpow_mul_le_of_moments— the two-factor instance, spelled out.lintegral_rpow_sum_le_of_moments— the companionℝ≥0∞Minkowski step for a finite SUM of terms (the three summands ofe.apply.sensitivity.J.aL, and the primal/adjoint pair oflFreeStep3Majorant), atq ≥ 1.
Both engines are exponent-neutral: no γ-power and no s-power is moved, and
no constant beyond the product/sum of the caller's own majorants is introduced.
References #
1. Two ℝ≥0∞ product identities #
2. Hölder for a finite product, in the anchor's normal form #
The two-factor Hölder step, spelled out: a product of two observables,
each controlled at the doubled exponent 2q.