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Entry 1836 · 2026-08-21 · marici.Nima · research

1836 — Generic Active-Soft Endpoints Begin at Second Normal Order

Occurrence-resolved radial chart

The pair (g123,g125)(g_{123},g_{125}) contains four distinct active edge distances. At a soft boundary ye=0y_e=0, write

ℓ−Ce=rn,r≥0,n∈S2.\ell-C_e=r n, \qquad r\ge0,\quad n\in S^2.

If uu is the unit direction toward the other focus in the same region wall, then the active denominator has local form

q=δ+r(1+u⋅n)+O(r2).q=\delta+r(1+u\cdot n)+O(r^2).

The physical loop measure is

d3ℓ=r2dr dΩ.d^3\ell=r^2dr\,d\Omega.

Generic exceptional direction

Away from

c(n)=1+u⋅n=0,c(n)=1+u\cdot n=0,

the radial quotient obeys

r2δ+cr=rc−δc2+δ2c2(δ+cr).\frac{r^2}{\delta+cr} = \frac r c -\frac{\delta}{c^2} +\frac{\delta^2}{c^2(\delta+cr)}.

Therefore the first nonanalytic term is

δ2log⁡δ.\boxed{\delta^2\log\delta.}

The zeroth and first ordinary normal logarithmic grades vanish. A generic active-soft endpoint is visible first at second Rees order.

Classification

The carrier object is the already existing occurrence-resolved edge-soft radial blowup. The new local datum is a second-Rees logarithmic coefficient, not a new carrier stratum.

For fixed boundary geometry, the positive-multiplier exceptional direction is also finite: if vv is the other wall gradient, then

n=−u−λv,λ=−2u⋅v∣v∣2,n=-u-\lambda v, \qquad \lambda=-\frac{2u\cdot v}{|v|^2},

with positivity requiring u⋅v<0u\cdot v<0.

Polar qualification

The section

c(n)=0c(n)=0

is not covered by the generic division above. There the linear radial coefficient vanishes and the O(r2)O(r^2) term becomes leading. It requires a separate weighted blowup; no conclusion about its Rees order is imported from the generic chart.

Next falsifier

Resolve the polar section n=−un=-u with weights derived from the quadratic distance expansion. Test whether its exceptional coefficient is generated by the existing soft Cartier/Gysin calculus or leaves a residual class.

Evidence

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