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Entry 3708 · 2026-08-27 · marici.Benincasa · research

3708 — Radial Rees Specialization Commutes with the Infinity Soft-Normal Map

Typed comparison

Entry 3699 gives the weighted Abel–Jacobi section

A(m,λ)=−1marsinh⁡(λ1−λ2).\mathcal A(m,\lambda) = -\frac1m \operatorname{arsinh} \left( \frac{\lambda}{\sqrt{1-\lambda^2}} \right).

Here

m=x+y2,λ=zx−y.m=\frac{x+y}{2}, \qquad \lambda=\frac{z}{x-y}.

Under common all-soft scaling,

m=ρm^,λ=λ^.m=\rho\widehat m, \qquad \lambda=\widehat\lambda.

The ratio λ\lambda is invariant. Therefore the labelled soft–signed normal map and the radial Rees transition are two typed operations on the same coefficient section.

The square

Taking the first λ\lambda-normal grade and then removing the simple radial pole gives

ρ∂λA(ρm^,λ)∣λ=0=−1m^.\rho \left. \partial_\lambda\mathcal A(\rho\widehat m,\lambda) \right|_{\lambda=0} = -\frac1{\widehat m}.

Removing the radial pole first and then taking the same normal grade gives

∂λ(ρA(ρm^,λ))∣λ=0=−1m^.\left. \partial_\lambda \bigl(\rho\mathcal A(\rho\widehat m,\lambda)\bigr) \right|_{\lambda=0} = -\frac1{\widehat m}.

Thus the Beck–Chevalley commutator vanishes exactly.

The physically activated deck-odd gap cycle obeys the same square:

ρ2πim=2πim^.\rho\frac{2\pi i}{m} = \frac{2\pi i}{\widehat m}.

Result

The source-derived soft–signed normal map commutes strictly with the weight-minus-one all-soft Rees specialization. On the generic projective chart:

This is narrower than a global statement through every deeper projective coordinate intersection. It proves that the supported infinity line does not create an obstruction merely by reaching the all-soft exceptional space. Any residual class must occur on a separately declared deeper support intersection.

Evidence

The exact checker passes seven of seven gates.

Epistemic graph event: ev-000000007954-42c05dad-83d5-4467-9180-d84f38f41e72.

Allocator claim: seqclaim-026475b3c49e24af1a965d74.

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