Section 3: Local forms, finite constants, and stopping #
This file was automatically generated by Claude.
Formalization of blueprint Section 3, "Local forms, finite constants, and stopping"
(sec:reduction, lines 363-468) of blueprint/formalization_blueprint.tex.
Two fractional coordinates admit opposite perturbations, as in
blueprint lem:absolute, line 390.
Every extreme point of the reciprocal exponent polytope is Boolean.
Blueprint lem:absolute, line 390: the admissible reciprocal exponents
are precisely the convex hull of Boolean configurations with at most k ones.
In particular d = 4, k = 2 gives the source interpolation polytope.
Product identity used by positive Hölder interpolation, valid also for zero and infinite bases because every exponent is nonnegative.
Positive product-integral bounds form a convex set of nonnegative
exponents. This is the Hölder interpolation step of lem:absolute, line 392.
Blueprint lem:absolute, line 392: positive Boolean endpoint estimates
interpolate throughout the complete reciprocal-exponent polytope. The extended
nonnegative formulation includes zero and infinite integrals without division.
The two occupied real progression slots have Jacobian j - i,
as used by blueprint lem:absolute, line 388.
Normalized Lebesgue measure on a source interval, for the local Lp norms.
Equations
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The two-L1 endpoint in blueprint lem:absolute, line 388.
A two-coordinate measure-preserving map supplies a positive endpoint
bound, as in the torus argument of blueprint lem:absolute, line 394.
Blueprint lem:absolute, torus two-slot endpoint with constant one
for a multiplier bounded by one.
Abstract positive rank-two estimate obtained from the empty, singleton
and pair endpoints. This assembles the interpolation argument in lem:absolute.
The finite moment used for positive interpolation; an infinity slot contributes the constant one and is bounded by its essential supremum.
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The essential-supremum factor used at the infinite interpolation endpoint.
Equations
- TrilinearHT.Auto.interpolationInfinityFactor ν p f = if p = ⊤ then MeasureTheory.eLpNorm f ⊤ ν else 1
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The full Lp version of positive rank-two interpolation, including
infinity exponents and zero or infinite norms, used in blueprint eq:absolute.
Weighted version of the positive rank-two estimate. The three hypotheses are precisely the endpoint integrals proved in the three source settings.
Blueprint eq:absolute on every rational connected subtorus, with the
exact multiplier constant and all exponents in [1, ∞].
Blueprint eq:absolute on the real line: the normalized positive local
form is bounded for every exponent in [1, ∞] with reciprocal sum at most two.
Only boundedness and interval support of the kernel are needed.
Blueprint eq:absolute for the actual complex local kernel and inputs.
The nonnegative integral gives the intended interpretation even for infinite norms.
The complex local form is controlled by the positive local estimate.
This is the form of lem:absolute used in lem:finite-CN.
Coordinate partial derivative of a local kernel. This keeps the source's total-order derivative convention rather than replacing it by an operator norm.
Equations
- TrilinearHT.Auto.localKernelPartial m n w z = iteratedDeriv m (fun (x : ℝ) => iteratedDeriv n (fun (t : ℝ) => w (x, t)) z.2) z.1
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Smoothness, interior support, four zero marginals, and the quantitative
derivative bounds in blueprint eq:local and eq:marginals, lines 371–376.
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Uniform pointwise bound supplied by the zeroth-order kernel estimate.
Equations
- TrilinearHT.Auto.localKernelSupBound κ = (κ.derivativeConstant * 2) ^ (κ.derivativeConstant * 2)
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The complete finite data quantified over by blueprint eq:CN: one
dyadic grid, a finite collection in at most N consecutive depths, an admissible
kernel at every selected cell, and compactly supported measurable Lq inputs.
- grid : RealDyadicGrid
Dyadic grid supporting the finite-depth local form.
Finite collection of dyadic cells used in the local form.
- firstDepth : ℤ
First permitted depth in the finite-depth window.
Local kernel assigned to each dyadic cell.
- admissible (c : ℤ × ℤ) : c ∈ self.cells → IsAdmissibleLocalKernel κ (dyadicGridLeft self.grid c.1 c.2) (dyadicGridLength self.grid c.1) (self.kernel c)
The four measurable, compactly supported inputs to the local form.
- measurable_input (i : Fin 4) : Measurable (self.input i)
- memLp_input (i : Fin 4) : MeasureTheory.MemLp (self.input i) (ENNReal.ofReal q) MeasureTheory.volume
- compact_input (i : Fin 4) : HasCompactSupport (self.input i)
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The finite numerator in blueprint eq:CN.
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- One or more equations did not get rendered due to their size.
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The nonnegative maximal-product denominator in blueprint eq:CN.
Equations
- TrilinearHT.Auto.finiteDepthDenominator D = ∫⁻ (x : ℝ), ∏ i : Fin 4, TrilinearHT.Auto.scalarMaximalQ q (D.input i) x
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Only strictly positive finite denominators enter the real ratios in
blueprint eq:CN, lines 398–403.
Equations
- One or more equations did not get rendered due to their size.
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The least constant at least one from blueprint eq:CN. Inserting one
before the supremum includes the empty-ratio case without a division convention.
Equations
- TrilinearHT.Auto.finiteDepthConstant κ q N = sSup (insert 1 (TrilinearHT.Auto.finiteDepthRatios κ q N))
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Every normalized local Lq norm is bounded by the source's uncentered
M_q at every point of the interval, as used in lem:finite-CN, line 409.
The uniform real constant furnished by the fixed admissible kernel class.
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The local L2 estimate followed by normalized exponent monotonicity,
the first step of blueprint lem:finite-CN, line 409.
The source local form is bounded pointwise on its interval by the product of the four uncentered maximal functions.
Blueprint lem:finite-CN, line 409: disjoint depth summation gives the
uniform linear-in-depth bound before the absorption argument begins.
Blueprint eq:CN and lem:finite-CN: the real supremum is bounded,
and the inserted value one enforces the required normalization.
Blueprint eq:CN: the defining inequality holds at the real supremum,
including zero and infinite denominator cases.
Blueprint eq:CN: every admissible real constant at least one majorizes
the constructed constant.