Reverse single-scale power comparison #
Equation (5.71) also gives the comparison in the direction needed by the final single-scale assembly. The price is the square of the off-path inverse parent-scale ratios. This file bounds that product by the uniform loss from (5.69), and packages the subsequent insertion of the full ratio cube.
The branch-scale power on the left of paper (5.72).
Equations
- Anderson4D.singleScaleBranchPower Nm mu compound = ∏ v ∈ t.BranchNodes, ↑(Anderson4D.scaleN Nm v) ^ (-2 * (↑(Anderson4D.gamma2 mu compound v) - 1))
Instances For
The leaf-scale power on the right of paper (5.72), including the distinguished-parent factor.
Equations
- One or more equations did not get rendered due to their size.
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The residual product in (5.71), specialized to the dyadic marking.
Equations
Instances For
Every off-path branch is a non-root branch.
On a non-root branch, the inverse parent-scale ratio is at least one.
The off-path inverse-ratio product is bounded by the product over all non-root branches.
Uniform (8 exp 4)^m bound for the residual product in (5.71).
Exact reverse form of (5.71): the leaf power is the branch power times the square of the residual off-path inverse-ratio product.
The closure direction needed after the copy elimination:
leafPower ≤ (8 exp 4)^(2m) * branchPower.
Consumable final form: after reversing (5.72), reinsert the full cube of
parent-scale ratios at total cost (8 exp 4)^(5m).