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LeanPool.Superdiffusion.Algsuperdiff.Section4.Provider.MinimalScale.KickSplit

KickSplit #

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

The clamp split of a two-term (Γ₂, Γ_{1/2}) display #

This module supplies the decomposition that meets both demands at once. Given a nonnegative X with a two-term display X ≤ 𝒪_{Γ₂}(A₁) + 𝒪_{Γ_{1/2}}(A₂), the two legs are the clamp and the overshoot at the deterministic threshold

lam := 8 A₁ ρ ,      ρ := (A₁/A₂)^{1/3}  (equivalently ρ³A₂ = A₁) ,
min(X, lam) ≤ 𝒪_{Γ₂}(8A₁) ,      X − min(X, lam) ≤ 𝒪_{Γ_{1/2}}(8A₂) .

Both legs are measurable functions of X alone, so they inherit verbatim every independence property of X: this is what makes provable rather than assumed. A split built from the two Γ-witnesses of the display instead would lose it, because the witnesses are supplied by the Section 3 anchor as bare existentials with no locality.

Why the threshold is at (A₁/A₂)^{1/3} #

ρ is the crossover of the two tails, and the exponent 1/3 is forced. The Γ₂ leg needs the Γ_{1/2} witness to be negligible on levels below lam, which costs √(A₁/A₂ · t) ≥ t² for t ≤ ρ, i.e. ρ³ ≥ ρ⁴/ρ; the Γ_{1/2} leg needs the Γ₂ witness to be negligible on levels above lam, which costs (lam/A₁)² ≥ √t for t up to ρ⁴. The two demands meet exactly at ρ ≍ (A₁/A₂)^{1/3}; the numerical factor 8 is what makes both hold with room to spare, and the proof below exhibits that room (15 t² ≥ log 2 and 15 √t ≥ log 2).

Main results #

ρ is a free parameter constrained only by ρ³A₂ = A₁, so no root is ever formed: the caller supplies ρ (in KickTails.lean, as (A₁/A₂)^{1/3}).

Scope #

Carrier-free: generic in the measure space.

References #

rpow bookkeeping at the two Orlicz indices #

The Γ₂ leg: the clamp #

The Γ₂ leg X^{(1)} = min(X, 8A₁ρ). Below the threshold the Γ_{1/2} witness is negligible against a Γ₂ tail, and above it the clamp makes the tail event empty.

The Γ_{1/2} leg: the overshoot #

The Γ_{1/2} leg X^{(2)} = X − min(X, 8A₁ρ). Above the threshold the Γ₂ witness is negligible against a Γ_{1/2} tail: at levels below ρ⁴ the constant part 4ρ of the normalized level already dominates √t, and above ρ⁴ the growing part 4t/ρ³ does.