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LeanPool.Superdiffusion.Algsuperdiff.Section4.Provider.Regularity.StepSevenVolume

StepSevenVolume #

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

t.regularity Step 7c: the hvol producer at the general triadic ratio #

The gap this module closes #

The composition gaps open with hvol: stepSevenGradientWithShom takes the volume cost

  gradLoc  ≤  3^{(d/2)(n'-n)} · gradCore

as a hypothesis, and no producer exists at that literal shape. The obstruction is a side condition: the manuscript asserts the inclusion

Since (z + □_n) ∩ □_m ⊆ U_{n'-2}, passing to the smaller set costs a volume factor 3^{(d/2)(n'-n)}

and the inclusion of the two truncated windows at scales n+1 and n'-2 needs n + 1 ≤ n' - 2, which appears in NO binder of the printed display and in no binder of stepSevenGradientWithShom.

  n + 3 ≤ n'      ↔      n + 1 ≤ n' - 2 ,

so the unstated hypothesis is free at the consumption site. The arithmetic is tight: the printed selection range [n+3, m-3] is what makes the Caccioppoli core at n'-2 contain the window at n+1; had the manuscript written [n+2, m-3] the display would be false as printed.

What is produced #

The masses IS ≤ IT remain the caller's: ν^{1/2}‖∇u‖_{L²(S)} is read as the symmetric coefficient energy, and its monotonicity in the domain is an integral monotonicity, not an estimate. No new estimate is derived here; every step is a proved atom or Real.rpow arithmetic.

References #

1. The side condition, and the inclusion it unlocks #

The tex's own inclusion (z+□_{n+1}) ∩ □_m ⊆ (z+□_{n'-2}) ∩ □_m, at the derived side condition.

2. The two volume bounds #

3^{d j} = (3^j)^d in the rpow spelling the volume comparison uses.

The window's volume lower bound (lower half). For z ∈ □_m and k - 1 ≤ m, the truncated window (z+□_k) ∩ □_m contains a full translate of □_{k-1} — the inscribed well-placed cube — so its volume is at least 3^{d(k-1)}. At k = n+1 this is the printed 3^{dn}.

The window's volume upper bound ((b), upper half). The truncated window sits inside the full translate z + □_j, whose volume is 3^{dj}.

The volume upper bound, moved from the core scale n'-2 up to the printed n'.

3. The general-ratio producer #

hvol at the general triadic ratio ((b)).

For z ∈ □_m, n ≤ m, and any two masses with IS ≤ IT carried by the window (z+□_{n+1}) ∩ □_m and the Caccioppoli core (z+□_{n'-2}) ∩ □_m, the volume-normalized square roots compare at the printed factor:

  √(IS/|S|)  ≤  3^{(d/2)(n'-n)} · √(IT/|T|) .

This is normalizedSqrt_le_volumeRatio_mul composed with sqrt_volumeRatio_le_rpow_three at the two window volume bounds above — the two halves, now with both of them supplied rather than assumed. The mass monotonicity IS ≤ IT is the caller's integral comparison and is the only input.