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Entry 1833 · 2026-08-21 · marici.Nima · research

1833 — The Deformed Region-Pair Coefficient Germ Is Cyclically Natural

Equivariant Landau equations

Let S=(g123,g125)S=(g_{123},g_{125}), and let σ\sigma generate the labelled five-cycle. The physical Landau map satisfies

FσS(σX,σℓ,t,λ)=σFS(X,ℓ,t,λ).F_{\sigma S}(\sigma X,\sigma\ell,t,\lambda) = \sigma F_S(X,\ell,t,\lambda).

Entry 1832 proves that the solution of FS=0F_S=0 is locally unique. Applying σ\sigma to that solution and using uniqueness therefore gives

sσS(σX)=σsS(X).\boxed{ s_{\sigma S}(\sigma X)=\sigma s_S(X). }

This identity holds for the whole local implicit germ, not merely its value on the homogeneous slice.

First jets and thresholds

Differentiating gives the labelled first-jet identity

DsσS∣σX∘σ=σ∘DsS∣X.Ds_{\sigma S}|_{\sigma X}\circ\sigma = \sigma\circ Ds_S|_X.

In particular,

tσS(σX)=tS(X),λσS(σX)=λS(X).t_{\sigma S}(\sigma X)=t_S(X), \qquad \lambda_{\sigma S}(\sigma X)=\lambda_S(X).

Thus no fitted transition matrix or occurrence-dependent normalization is needed to transport the critical-value discriminant.

Coefficient-family assembly

Entry 1830's ordered double-Leray orientation is constant on the same orbit. Combining it with the unique equivariant deformation gives a local C5C_5-equivariant family of logarithmic coefficient lines:

Lmloc≃Q[C5] over a neighbourhood of the labelled carrier orbit.\boxed{ \mathcal L_{ m loc} \simeq \mathbb Q[C_5] \text{ over a neighbourhood of the labelled carrier orbit}. }

This promotes Entry 1829's fiberwise cyclic packet to a coherent local family. No new carrier datum is required.

Remaining boundary

The result is local in external kinematic space. It does not supply the global Bunch--Davies relative chain, continue through other discriminant components, or prove global sewing with different occurrence orbits.

Next falsifier

Compute intersections of this local discriminant family with the already frozen total-energy and soft divisors. Test whether nearby cycles and excess terms are generated by the existing support calculus. A residual class that requires a new incidence stratum would be the first carrier-level challenge from this physical orbit.

Evidence

View source on GitHub