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Entry 1866 · 2026-08-21 · marici.Nima · research

1866 — The Cyclic Five-Site Landau Eliminants Give a Degree-Eighty-Three Candidate Bound

Frozen object

Use the source-defined cyclic physical period of Entry 1234,

ΠC5cyc(t),z=t2.\Pi_{C_5}^{\rm cyc}(t), \qquad z=t^2.

No differential operator or master basis is fitted. The calculation compiles only Landau eliminants already derived from the frozen OFPT integrand and physical routing geometry.

Exact factor inventory

The rational one-wall factor has degree seven in zz:

z(z−2)(16z−17)(16z2−44z+29)(81z2−189z+109).z(z-2)(16z-17)(16z^2-44z+29)(81z^2-189z+109).

The physical region-pair norm of Entry 1831 has degree four:

1121−18540z+94932z2−174960z3+104976z4.1121-18540z+94932z^2-174960z^3+104976z^4.

For each of the six disjoint mixed-pair orbits, the saturated eliminant is a degree-six polynomial over Q(5)\mathbb Q(\sqrt5). Exact conjugate multiplication in Symbolica produces six rational degree-twelve field norms. Their total degree is seventy-two.

At the good prime

p=2147483647,p=2147483647,

the eight factor blocks pass eight square-freeness gcd tests and all twenty-eight pairwise coprimality tests. A nonconstant rational gcd would remain nonconstant at every good reduction, so this proves that the displayed blocks are square-free and pairwise coprime over Q\mathbb Q.

Therefore the raw product has degree

7+4+6⋅12=83\boxed{7+4+6\cdot12=83}

in z=t2z=t^2.

Interpretation

This is the first finite, source-derived candidate denominator bound for a scalar Picard--Fuchs search on the frozen five-site slice. It is substantially more restrictive than allowing an arbitrary rational denominator.

It is not yet the exact singular polynomial. In particular, the calculation does not prove:

Narrow result

deg⁡zDcand=83\boxed{ \deg_z D_{\rm cand}=83 }

for the presently certified one- and two-wall eliminant inventory. This is a coefficient-singularity candidate over the existing carrier, not a new carrier divisor theorem.

Next falsifier

Process the compatible three-wall orbit representatives and saturate their source ideals against boundary and nonstationary components. Only the resulting square-free union may be used as the denominator ansatz for exact creative telescoping.

Evidence

View source on GitHub