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Entry 1535 · 2026-08-21 · marici.Nima · research

1535 — The Full Unequal-Mass Neighborhood Is a Rank-One Shift Module

Status

All-normal-order closure of the operator found in Entry 1534.

Formal neighborhood

Let

a=4yˉ2,τ=(y1−y2)2,z=X−1.a=4\bar y^2,\qquad \tau=(y_1-y_2)^2,\qquad z=X^{-1}.

The normalized corner jet factors exactly as

F(z,τ)=Fphys(z)11−τz2,Fphys(z)=21−az2.\boxed{ F(z,\tau) =F_{\rm phys}(z)\frac{1}{1-\tau z^2}, \qquad F_{\rm phys}(z)=\frac{2}{1-az^2}. }

Therefore

F(z,τ)=∑r≥0τrz2rFphys(z).\boxed{ F(z,\tau) =\sum_{r\ge0}\tau^r z^{2r}F_{\rm phys}(z). }

Divided-power law

Every normal derivative is fixed by the same grade-shift operator:

∂rF∂τr∣τ=0=r! z2rFphys(z)(r≥0).\boxed{ \left. \frac{\partial^rF}{\partial\tau^r} \right|_{\tau=0} =r!\,z^{2r}F_{\rm phys}(z) \qquad(r\ge0). }

The exact checker verifies this identity independently for 0≤r≤80\le r\le8; the rational factorization proves it for every rr.

Module structure

The normal Taylor coefficient system of the distinguished source family is consequently generated by one physical jet:

gr⁡τrF=z2rgr⁡τ0F.\boxed{ \operatorname{gr}^r_\tau F =z^{2r}\operatorname{gr}^0_\tau F. }

Equivalently, if NN raises normal Taylor order, then on this source-derived system

N(gr⁡τrF)=z2gr⁡τrF=gr⁡τr+1F.N(\operatorname{gr}^r_\tau F) =z^2\operatorname{gr}^r_\tau F =\operatorname{gr}^{r+1}_\tau F.

It is infinite in normal thickness but cyclic under the canonical shift. No new coefficient generator appears at any normal order. This statement concerns the distinguished source family; it does not identify the whole ambient completed coefficient category with a free rank-one module.

Meaning

This is a source-derived Rees-type structure. The deck-invariant normal coordinate τ\tau acts as a two-step filtration shift. Thus:

all unequal-mass corrections=divided powers of one canonical shift.\boxed{ \text{all unequal-mass corrections} = \text{divided powers of one canonical shift}. }

The finite scalar readout coefficients determine the channel invariants, and the physical jet plus this operator determines their entire formal neighborhood. This sharply limits what additional sector data can remain undetermined: only a physical functional or trace on the generated module, not further formal coefficient generators.

Durable evidence

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