The power ledger in paper equation (5.71) #
This file lifts the nodewise exponent identity already proved in
SingleScaleSetup to the direct finite-product identity used in Step 1 of
Proposition 5.10. The distinguished leaf is kept explicit.
Branch nodes whose subtree does not contain the distinguished leaf.
Equations
- Anderson4D.branchesOffLeafPath l₀ = {v ∈ t.BranchNodes | ¬↑v <+: ↑↑l₀}
Instances For
A branch child is off the distinguished path exactly when its subtree does not contain the distinguished leaf.
Equations
- Anderson4D.branchChildrenOffLeafPath v l₀ = {c ∈ Anderson4D.branchChildren v | ¬↑c <+: ↑↑l₀}
Instances For
Collected exponent of one branch scale in the last ratio product of paper (5.71).
Equations
- Anderson4D.branchesOffLeafPathRatioExponent v l₀ = ↑(Anderson4D.branchChildren v).card - ↑(Anderson4D.branchChildrenTowardLeaf v l₀).card - if ↑v <+: ↑↑l₀ then 0 else 1
Instances For
The final ratio product in (5.71), regrouped as one integer power at every branch node.
The uncollected right side of (5.71) equals the product carrying the
nodewise exponent paper571RhsExponent.
Paper equation (5.71) in direct finite-product form.
Paper (5.72)'s power inequality. Squaring the inverse of (5.71) leaves an extra negative square of the off-path parent ratios; it is at most one because branch scales increase toward the root.
Specialization of the (5.72) power ledger to the dyadic Hepp marking.
Quantitative form of the first reduction after (5.69): the missing cube of the parent-scale-ratio product can be inserted at exponential cost.