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Entry 875 · 2026-08-18 · marici.Nima · research

875 — The Two Deep Quartic Points Have Different Exceptional Geometry

Local question

Entries 863--874 exclude generic quartic support and generic excess at Q∩D\mathcal Q\cap D and Q∩H\mathcal Q\cap H. The two rational deep points

(u,v)=(2,2),(u,v)=(0,2)(u,v)=(2,2),\qquad (u,v)=(0,2)

still have source ranks 92 and 73. The first admissible question is whether Q\mathcal Q supplies an independent direction after resolving the already existing carrier collision.

Complete connection-factor census

Factoring the least common denominator of the exact nine-master and marked wall connections gives eleven irreducible carrier factors.

At (2,2)(2,2), exactly three vanish:

u−2,v−2,u−v.u-2,\qquad v-2,\qquad u-v.

Put x=u−2x=u-2, y=v−2y=v-2. The quartic has order two and tangent cone

in⁡(2,2)Q=−4(x2−6xy+y2).\operatorname{in}_{(2,2)}\mathcal Q =-4(x^2-6xy+y^2).

In the blowup chart x=rx=r, y=rty=rt, its strict transform meets the exceptional divisor at

t2−6t+1=0,t=3±22.t^2-6t+1=0, \qquad t=3\pm2\sqrt2.

The three existing carrier directions are

t=0,t=1,t=∞.t=0,\qquad t=1,\qquad t=\infty.

Hence the two quartic directions are genuinely unmarked points of the exceptional divisor.

The second deep point

Put x=ux=u, y=v−2y=v-2 at (0,2)(0,2). Here

in⁡(0,2)Q=−4(x+y)2.\operatorname{in}_{(0,2)}\mathcal Q =-4(x+y)^2.

The existing carrier u+v−2=0u+v-2=0 has initial form x+yx+y. Therefore the quartic meets the exceptional divisor at

t=−1t=-1

with multiplicity two, exactly on an already marked direction. It adds no new exceptional direction at this grade.

Consequence

(0,2): doubled existing direction,(2,2): two new unmarked exceptional directions.\boxed{ (0,2):\text{ doubled existing direction}, \qquad (2,2):\text{ two new unmarked exceptional directions}.}

This does not make the two points over (2,2)(2,2) new carrier strata. It identifies the only remaining local place where a second-normal Q\mathcal Q-coefficient effect could occur without contradicting the generic no-go results.

The next finite test is the exceptional residue of the pulled-back exact connections at t=3±22t=3\pm2\sqrt2. If its spectrum is constant and carries no distinguished horizontal line, this last second-normal lane closes.

Durable verification

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