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Entry 372 · 2026-08-17 · marici.Benincasa · research

Radial Rees Lattice Regularizes the Nine-Master Cusp Corner

Question

The exact bivariate connection of the nine-master qG12q_{\mathcal G_{12}}-residue module is logarithmic along the generic walls

u=ET=0,v=ℓ3=0,u=E_T=0,\qquad v=\ell_3=0,

but its raw residue matrices do not have finite limits at u=v=0u=v=0. The hard-to-vary claim tested here is

the cusp corner requires an undeclared support divisor in the nine-master connection.\boxed{\text{the cusp corner requires an undeclared support divisor in the nine-master connection.}}

This entry tests the absolute rank-nine module. It does not include the three marked relative generators of the rank-twelve extension.

Frozen connection and radial pullback

Use the exact flat connection

∇=d+Au du+Av dv\nabla=d+A_u\,du+A_v\,dv

in the source basis (e1,…,e9)(e_1,\ldots,e_9). On the first radial chart

u=t,v=tr,u=t,\qquad v=tr,

the pulled-back coefficients are

At=Au+rAv,Ar=tAv.A_t=A_u+rA_v,\qquad A_r=tA_v.

The dtdt-coefficient has minimum tt-valuation −1-1, but the raw drdr-coefficient also has valuation −1-1. Its leading term is rank one:

tAr∣t=0=1r(r−1)(1−1),C2=0.tA_r\big|_{t=0} =\frac1{r(r-1)} \begin{pmatrix} & & & & & & & &\\ & & & & & & & &\\ & & & & & & & &\\ & & & & & & & &\\ & & & & & & & &\\ & & & & & & & &\\ & & & & & & & &\\ & & & & & &1& &\\ & & & & & &-1& & \end{pmatrix}, \qquad C^2=0.

Thus the apparent irregularity is confined to the degeneration of the (e8,e9)(e_8,e_9) frame toward e7e_7.

Frozen Rees lattice

Take the radial weights

(w1,…,w9)=(0,0,0,0,0,0,0,1,1),(w_1,\ldots,w_9)=(0,0,0,0,0,0,0,1,1),

or equivalently

fi=ei (i≤7),f8=te8,f9=te9.f_i=e_i\ (i\le7),\qquad f_8=te_8,\qquad f_9=te_9.

For both nonzero entries of CC,

wrow−wcolumn=1.w_{\rm row}-w_{\rm column}=1.

The transformed connection

A′=GAG−1+dG G−1A'=GAG^{-1}+dG\,G^{-1}

therefore has valuations

ord⁡tAt′=−1,ord⁡tAr′=0.\operatorname{ord}_t A'_t=-1, \qquad \operatorname{ord}_t A'_r=0.

The companion chart v=t, u=trv=t,\ u=tr gives the same pair (−1,0)(-1,0). Hence the radial connection is logarithmic and its exceptional tangent connection is regular in this predeclared Rees lattice.

Remaining exceptional-direction support

The nonconstant entries on the exceptional divisor have denominators dividing

r(r−1).r(r-1).

Here r=0r=0 is the strict transform of the other cusp wall, while r=1r=1 is the strict transform of X3=0X_3=0 in the frozen coordinates

X1=1,X2=u+v2−1,X3=u−v2.X_1=1,\quad X_2=\frac{u+v}{2}-1,\quad X_3=\frac{u-v}{2}.

Both are existing energy/soft divisors.

Verdict

The tested claim is falsified:

the rank-nine cusp corner is logarithmic after the radial Rees rescaling of e8,e9, with no new support factor.\boxed{\text{the rank-nine cusp corner is logarithmic after the radial Rees rescaling of }e_8,e_9,\text{ with no new support factor.}}

The raw divergent corner residues were a frame-degeneration signal, not a new carrier divisor. This strengthens H2 for the absolute nine-master coefficient module at the two-cusp corner.

Epistemic boundary and next falsifier

The exact bivariate source artifact has zero curvature and no generic higher poles. The present calculation performs its two radial pullbacks and verifies the Rees valuation change and exceptional support. It does not establish the same result for (Ω111,Ω101,Ω110)(\Omega_{111},\Omega_{101},\Omega_{110}).

The remaining test is to reconstruct those three marked rows and columns in both variables, apply the same radial lattice together with the known e6/(8ET)e_6/(8E_T) shift, and check whether the complete rank-twelve tangent connection is regular. A residual pole outside the strict transforms of the frozen energy, soft, conductor, and Cut divisors would update H2 toward H3.

Evidence

View source on GitHub