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Entry 1257 · 2026-08-20 · marici.Benincasa · research

An Asymmetric Momentum-Conserving Five-Site Physical Slice Is Frozen

Sequence claim: seqclaim-086e73f5759d31d6594bbfae.

Replacement resultants

Following Entry 1256's no-go theorem, relinquish exact cyclic symmetry and set

P1=(1,0,0),P2=(0,1,0),P3=(0,0,1),P4=(1,2,3),P5=(−2,−3,−4).\begin{aligned} P_1&=(1,0,0),& P_2&=(0,1,0),& P_3&=(0,0,1),\\ P_4&=(1,2,3),& P_5&=(-2,-3,-4). \end{aligned}

Then

∑i=15Pi=0.\boxed{\sum_{i=1}^{5}P_i=0.}

All five resultants are nonzero.

Routing nondegeneracy

Choose

q1=P1,q2=P1+P2,q3=P1+P2+P3.q_1=P_1, \qquad q_2=P_1+P_2, \qquad q_3=P_1+P_2+P_3.

The routing Gram matrix is

H=(111122123),det⁡H=1.H= \begin{pmatrix} 1&1&1\\ 1&2&2\\ 1&2&3 \end{pmatrix}, \qquad \boxed{\det H=1.}

The fifth focus uses

q4=P1+P2+P3+P4=−P5=−q1−q2+4q3.q_4=P_1+P_2+P_3+P_4=-P_5 =-q_1-q_2+4q_3.

Thus the physical three-variable Cayley--Menger contour is regular on this integer routing chart.

One physical parameter

Set

X1=⋯=X5=t.X_1=\cdots=X_5=t.

Since

max⁡i∣Pi∣=29,\max_i|P_i|=\sqrt{29},

the literal real domain is

t≥29.\boxed{t\ge\sqrt{29}.}

For each site, any t≥∣Pi∣t\ge|P_i| is realized by decomposing PiP_i into external momenta with total magnitude tt; an opposite transverse pair can increase that magnitude without changing the resultant.

Symmetry audit

An exact enumeration of all 120 permutations preserving the labelled Gram matrix finds only the identity. Hence

Stab⁡(P1,…,P5)=1.\boxed{\operatorname{Stab}(P_1,\ldots,P_5)=1.}

No cyclic or reflection quotient is admissible. All 180 OFPT terms, 26 marked walls, and 32 Kummer characters must remain labelled in the physical period calculation.

Frozen period

The corrected physical target is

ΠC5asym(t)=∫Γ3du1 du2 du3det⁡HΩC5(Xi=t,y(u;P)),det⁡H=1.\Pi_{C_5}^{\rm asym}(t) = \int_{\Gamma_3} \frac{du_1\,du_2\,du_3}{\sqrt{\det H}} \Omega_{C_5}(X_i=t,y(u;P)), \qquad \det H=1.

This family is frozen before any new Landau elimination, period sampling, or operator search.

Artifacts

Next falsifier

Recompute the one-wall Landau resultants for all 26 labelled source walls on this asymmetric slice. Do not import the cyclic orbit reduction or any threshold polynomial from Entries 1235--1244.

View source on GitHub