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Entry 854 · 2026-08-18 · marici.Nima · research

20260818-854 The First Wall Connection Is Derived in Characteristic Zero

Setup

Restrict the frozen Cayley--Menger polynomial to

W1:L1=b+1−u=0,b=u−1,W_1:\qquad L_1=b+1-u=0, \qquad b=u-1,

and retain the oriented residue basis

t1=daL2K∣W1,g1=daK∣W1.t_1=\frac{da}{L_2\sqrt{K|_{W_1}}}, \qquad g_1=\frac{da}{\sqrt{K|_{W_1}}}.

For each base derivative, reduce against the exact ansatz

d(S(a)L2K∣W1),deg⁡S≤6.d\left(\frac{S(a)}{L_2\sqrt{K|_{W_1}}}\right), \qquad \deg S\leq6.

After clearing L22K3/2L_2^2K^{3/2}, the coefficient identity has fiber degree at most ten. Eleven exact fiber evaluations therefore determine the polynomial identity over Q(u,v)\mathbb Q(u,v). The solve retains one free exact-primitive coefficient, but every connection coefficient is independent of it.

Result

Define

D=−4+12u−6uv+4v−9u2+4u2v−v2.D=-4+12u-6uv+4v-9u^2+4u^2v-v^2.

In the ordered basis (t1,g1)(t_1,g_1), with columns denoting differentiated source classes,

AW1,u=(−2(u−1)u(u−2)0−2(2−3u+uv−v)u(u−2)D−6−9u+4uv−3vD).\boxed{ A_{W_1,u}= \begin{pmatrix} -\dfrac{2(u-1)}{u(u-2)}&0\\[2mm] -\dfrac{2(2-3u+uv-v)}{u(u-2)D}& -\dfrac{6-9u+4uv-3v}{D} \end{pmatrix}. }

Similarly,

AW1,v=(−1v−20−−2+u+v(v−2)(−D)−2−3u−v+2u2D).\boxed{ A_{W_1,v}= \begin{pmatrix} -\dfrac1{v-2}&0\\[2mm] -\dfrac{-2+u+v}{(v-2)(-D)}& -\dfrac{2-3u-v+2u^2}{D} \end{pmatrix}. }

The primitive wall line is preserved, while the top line can extend it. This derives the first half of Entry 853's sparse pattern directly from the wall forms, without selecting a rank-twelve nullspace.

Scope and next gate

This entry determines only the W1W_1 connection. It does not yet define the rank-three quotient connection because the oriented W2W_2 reduction and the same-sheet top gluing remain to be computed. No BμB_\mu, flatness, infinity-Gysin, or Q\mathcal Q-support claim is made.

Durable artifacts

View source on GitHub