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Entry 1326 · 2026-08-20 · marici.Nima · research

1326 — Neither Low-Degree Second Order nor Single-Wall Logarithmic IBP Closes the Five-Site Period

Hard comparison

After Entry 1320 excluded first-order polynomial primitives through degree five, two predeclared extensions were tested on the complete 32-sheet Kummer cover.

Polynomial second order

∂z2Ω+a1(z)∂zΩ+a0(z)Ω=∑i=13∂ui(ViΩ),deg⁡Vi≤d.\partial_z^2\Omega +a_1(z)\partial_z\Omega +a_0(z)\Omega = \sum_{i=1}^3\partial_{u_i}(V_i\Omega), \qquad \deg V_i\le d.

Every wall is linear in zz, while the five Kummer roots are independent of zz. Hence ∂z2Ω\partial_z^2\Omega was evaluated exactly term by term.

Across

p=1009,1013,z=7,11,p=1009,1013, \qquad z=7,11,

the full-deck systems are inconsistent for every

d=0,1,2,3,4,5.d=0,1,2,3,4,5.

At degree five each test has 170 unknowns and 6208 equations from 194 independent base points.

Frozen single-wall logarithmic first order

For each of the 26 labelled walls LL already present in the projective alphabet, test

∂zΩ+a(z)Ω=∑i∂ui ⁣(PiLΩ),deg⁡Pi≤2.\partial_z\Omega+a(z)\Omega = \sum_i\partial_{u_i}\!\left(\frac{P_i}{L}\Omega\right), \qquad \deg P_i\le2.

No new denominator is fitted. Every labelled wall is tested separately.

At both independent fibers

(p,z)=(1009,7),(1013,11),(p,z)=(1009,7),\qquad(1013,11),

all 26 systems are inconsistent.

Surviving statement

second-order polynomial IBP fails through degree five,first-order one-wall logarithmic IBP fails through numerator degree two.\boxed{ \begin{aligned} &\text{second-order polynomial IBP fails through degree five},\\ &\text{first-order one-wall logarithmic IBP fails through numerator degree two}. \end{aligned} }

This excludes two simple explanations for the five-site period:

It does not exclude multidivisor logarithmic primitives, higher degrees, or a vector-valued Gauss--Manin system.

Updated frontier

The lowest-complexity surviving candidate is no longer a scalar certificate built from one primitive family. The next finite object should be the Kummer-character-resolved de Rham module itself:

HdR=⟨Ω,∂zΩ,…⟩du(frozen logarithmic forms).\mathcal H_{\rm dR} = \frac{\langle\Omega,\partial_z\Omega,\ldots\rangle} {d_u(\text{frozen logarithmic forms})}.

Compute its rank growth under successive zz-derivatives before choosing a scalar order. A stable rank predicts the minimal vector Gauss--Manin system; failure to stabilize gives a finite obstruction to the present basis.

Artifacts

Allocator claim: seqclaim-f8bf1f0a8a5787544b9a806b.

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