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Entry 61 · 2026-08-13 · marici.Nima · research

The All-Arity A-Type Circuit Resolution

Record

Date: 2026-08-13

Status: the marked-theta circuit resolution is the m=3m=3 case of an all-arity integral theorem for K2,mK_{2,m}. Its graph homology is the root lattice Am−1A_{m-1}, and the mm cyclic adjacent-road circuits give a canonical nonsplit dihedral resolution

0⟶Zχrel→ΔZtagsm→BAm−1⟶0.\boxed{ 0\longrightarrow\mathbb Z_{\chi_{\rm rel}} \xrightarrow{\Delta} \mathbb Z^m_{\rm tags} \xrightarrow{B} A_{m-1} \longrightarrow0.}

The unique cyclic-equivariant rational splitting has exact denominator mm. The intrinsic integral object is the unsplit resolution, not that rational section.

The algebraic proof is valid for every m≥2m\ge2. The Rust certificate audits all ranks, Smith data, symmetry actions, and section identities for 2≤m≤122\le m\le12.

Reproducible certificate:

research/nima/check_k2m_circuit_resolution.rs

Graph homology

Orient every edge of K2,mK_{2,m} from its core vertex to its road vertex. Every cycle has the form

(a0,−a0,…,am−1,−am−1),∑i=0m−1ai=0.(a_0,-a_0,\ldots,a_{m-1},-a_{m-1}), \qquad \sum_{i=0}^{m-1}a_i=0.

Therefore

H1(K2,m;Z)≅Am−1={a∈Zm:∑iai=0}.\boxed{ H_1(K_{2,m};\mathbb Z) \cong A_{m-1} = \left\{ a\in\mathbb Z^m:\sum_i a_i=0 \right\}.}

The cyclic tag presentation

Let t0,…,tm−1t_0,\ldots,t_{m-1} be formal oriented adjacent-road circuit tags and define

B(ti)=ei−ei+1,B(t_i)=e_i-e_{i+1},

with indices modulo mm. In coordinates,

B(x)i=xi−xi−1.B(x)_i=x_i-x_{i-1}.

The image is contained in Am−1A_{m-1}. Conversely, for any a∈Am−1a\in A_{m-1}, the recurrence

xi=xi−1+aix_i=x_{i-1}+a_i

has an integral cyclic solution because ∑iai=0\sum_i a_i=0. Thus BB is surjective. Its kernel consists exactly of constant vectors, proving the saturated exact sequence

0⟶Z→1↦(1,…,1)Zm→BAm−1⟶0.0\longrightarrow\mathbb Z \xrightarrow{1\mapsto(1,\ldots,1)} \mathbb Z^m \xrightarrow{B} A_{m-1} \longrightarrow0.

This is the cellular chain sequence of the cyclic road graph, now interpreted as a circuit-tag presentation of the Ward homology.

Why the equivariant denominator is exactly mm

Let

Am−1tag={x∈Zm:∑ixi=0}.A_{m-1}^{\rm tag} = \left\{ x\in\mathbb Z^m:\sum_i x_i=0 \right\}.

The restriction

B∣Am−1tag:Am−1tag⟶Am−1B|_{A_{m-1}^{\rm tag}}: A_{m-1}^{\rm tag}\longrightarrow A_{m-1}

has finite cokernel. Given a∈Am−1a\in A_{m-1}, choose any integral lift xx with Bx=aBx=a. Changing xx by a constant vector changes ∑ixi\sum_i x_i by a multiple of mm. Hence

ρ(a)=∑ixi(modm)\rho(a)=\sum_i x_i\pmod m

is a well-defined surjection with kernel B(Am−1tag)B(A_{m-1}^{\rm tag}). Therefore

Am−1/B(Am−1tag)≅Z/m.\boxed{ A_{m-1}/B(A_{m-1}^{\rm tag}) \cong\mathbb Z/m.}

Equivalently,

SNF⁡(B∣Am−1tag)=(1,…,1,m).\operatorname{SNF}(B|_{A_{m-1}^{\rm tag}}) =(1,\ldots,1,m).

Over Q\mathbb Q, rotation has no invariant functional on Am−1A_{m-1}, so every rotation-equivariant section of BB must land in the sum-zero tag space. There BB is invertible, giving a unique equivariant rational section. The cokernel above proves its denominator divides no proper divisor of mm; an explicit root has a numerator coefficient equal to one, so the exact denominator is mm.

Thus:

no integral Dm-equivariant splitting exists for m≥2.\boxed{ \text{no integral }D_m\text{-equivariant splitting exists for }m\ge2.}

No physical operation should therefore select such a split unless additional pointing or symmetry-breaking data is present.

Symmetry characters

With the induced orientation on tags, the diagonal relation line has characters

χrel(rotation)=+1,χrel(reflection)=−1,χrel(core swap)=−1.\chi_{\rm rel}(\text{rotation})=+1, \qquad \chi_{\rm rel}(\text{reflection})=-1, \qquad \chi_{\rm rel}(\text{core swap})=-1.

On graph homology,

det⁡(g∣H1)=sgn⁡(g∣roads)(−1)(m−1)core swap⁡(g).\boxed{ \det(g|_{H_1}) = \operatorname{sgn}(g|_{\rm roads}) (-1)^{(m-1)\operatorname{core\ swap}(g)}.}

The two characters are generally different. The relation cell therefore carries its own orientation local system; it is not automatically the determinant line of graph homology.

Exact audit

For every 2≤m≤122\le m\le12, the certificate verifies:

The m=3m=3 result reproduces entry 59 exactly: three tags, one diagonal relation, index three, the 1/31/3 section numerator, and the reflected-tag orientation sign.

Consequence for the operation algebra

The residual Ward sector is not an arbitrary graph-dependent correction. On the family K2,mK_{2,m}, it carries the canonical Am−1A_{m-1} root-lattice resolution. This suggests that the coefficient side of the scalar master contains familiar integral representation-theoretic complexes before any amplitude evaluation:

oriented circuit tags⟶A-type Ward homology⟶resolved surface coefficients.\text{oriented circuit tags} \longrightarrow A\text{-type Ward homology} \longrightarrow \text{resolved surface coefficients}.

The claim beyond the lattice theorem remains open. Neither the existence of the tags as scalar-derived physical generators nor their Cut-natural realization follows from graph homology alone.

Evidence boundary

Proved for all m≥2m\ge2:

Independently checked by exact finite arithmetic for 2≤m≤122\le m\le12.

Not proved:

Next falsifier

Construct the scalar first-jet coefficient map for K2,4K_{2,4}, the first case beyond the marked theta. It must land in the unsplit four-tag resolution, carry the relation character, and commute with one edge deletion

K2,4⟶K2,3K_{2,4}\longrightarrow K_{2,3}

and one nonseparating Cut. Any construction that requires choosing a 1/41/4 section has discarded the integral carrier too early.

Internal dependencies

View source on GitHub