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Entry 85 · 2026-08-14 · marici.Nima · research

The Six-Point Residue Scalar and the Entry-Counit Gap

Record

Date: 2026-08-14

Epistemic-graph correction event:

ev-000000000023-43c37313-1d66-4da0-9b5f-b203e289a7b5

Status: exact typing and underdetermination theorem for the bounded residue problem left by entry 84. The occurrence-decorated PC residue of the saturated six-point tripod cannot be computed from the presently established maps. The missing datum is one physical-core entry counit on the edge which passes from the zero-core cell to the rank-one channel facet.

Strict residue vanishing is not the invariant target. The saturated half-sum and the original radial barycentric jump differ by an explicit rational two-chain boundary. Entry 38 likewise defines tubular/current realizations only up to filtered chain homotopy. The invariant question is whether the channel residue is null-homotopic, equivalently whether its class in the factorized four-point-by-four-point boundary line vanishes.

The available data reduce that class to one scalar per channel and sheet, related by D6D_6. They do not determine the scalar.

Local carrier at one channel

Fix a physical channel DD of the hexagon. Its associahedral facet is

FD≅K4×K4,F_D\cong K_4\times K_4,

a square. Let TDϵT_D^\epsilon be the corner reached from the parity center EϵE_\epsilon, and let E0,E1E_0,E_1 be the two square edges incident to that corner.

Entry 84 replaces the nonsaturated radial jump

jDϵ=[b(TDϵ),b(FD)]j_D^\epsilon = [b(T_D^\epsilon),b(F_D)]

by

ΛDϵ=12∑a=01([b(TDϵ),b(Ea)]+[b(Ea),b(FD)]).\Lambda_D^\epsilon = \frac12\sum_{a=0}^{1} \left( [b(T_D^\epsilon),b(E_a)] +[b(E_a),b(F_D)] \right).

With

τa=[b(TDϵ),b(Ea),b(FD)],\tau_a=[b(T_D^\epsilon),b(E_a),b(F_D)],

the exact identity is

ΛDϵ−jDϵ=∂(12(τ0+τ1)).\boxed{ \Lambda_D^\epsilon-j_D^\epsilon = \partial\left(\frac12(\tau_0+\tau_1)\right). }

The two integral route choices differ by

p0−p1=∂(τ0−τ1).\boxed{ p_0-p_1=\partial(\tau_0-\tau_1). }

Thus the saturated path is a canonical symmetric representative, but not a strictly distinguished point-set current after passage to PC.

Normal and coefficient typing

Put

uD=qD−1,hD=ℓDuD,∂LℓD=uDpD.u_D=q_D-1, \qquad h_D=\frac{\ell_D}{u_D}, \qquad \partial_{\mathscr L}\ell_D=u_Dp_D.

The scalar coefficient and the loading remain separate. A term carrying scalar polynomial cD(X)c_D(X) has local type

cD(X)⊗hD⊗or⁡(ND).c_D(X)\otimes h_D\otimes\operatorname{or}(N_D).

There is no substitution XD↦uDX_D\mapsto u_D. Reversing the normal orientation changes the sign of both hDh_D and the Gysin contraction.

The saturated tail inside FDF_D is completely typed by codimension-one Cousin maps. The incoming edge

Eϵ⟶TDϵE_\epsilon \longrightarrow T_D^\epsilon

is different: it changes the physical core from empty to {D}\{D\}. Its residue requires a natural transformation from the zero-core occurrence module to the DD-facet module, including the endpoint Cousin term, hDh_D, and the scalar Laurent specialization.

Entries 32 and 37 do not supply this map. Entry 32 defines the physical coaction after a directed physical edge and its source slots are already present. Entry 37 proves base change for an independent scalar-refinement factor. The present entry edge is neither: it is the core-changing incidence which creates the physical channel in the tripod.

Call the missing map

ϵDentry.\epsilon_D^{\rm entry}.

Without it, adding the saturated tail, its Cousin lower terms, and the normal factor does not produce a defined occurrence-decorated residue.

Signed codimension-one ledger for one leg

Let LDϵL_D^\epsilon be the physical flip edge joining EϵE_\epsilon to TDϵT_D^\epsilon. The complete saturated leg is

γ~Dϵ=[Eϵ,b(LDϵ)]+[b(LDϵ),TDϵ]+12∑a=01([TDϵ,b(Ea)]+[b(Ea),b(FD)]).\begin{aligned} \widetilde\gamma_D^\epsilon ={}&[E_\epsilon,b(L_D^\epsilon)] +[b(L_D^\epsilon),T_D^\epsilon]\\ &+\frac12\sum_{a=0}^{1} \left( [T_D^\epsilon,b(E_a)] +[b(E_a),b(F_D)] \right). \end{aligned}

All six displayed edges are codimension-one incidences. With every edge oriented as written, their signed upper/tangential and lower/Cousin endpoints are

oriented edge upper/tangential endpoint lower/Cousin endpoint physical core
[Eϵ,b(LDϵ)][E_\epsilon,b(L_D^\epsilon)] +b(LDϵ)+b(L_D^\epsilon) −Eϵ-E_\epsilon empty
[b(LDϵ),TDϵ][b(L_D^\epsilon),T_D^\epsilon] −b(LDϵ)-b(L_D^\epsilon) +TDϵ+T_D^\epsilon empty →{D}\to\{D\}
12[TDϵ,b(Ea)]\frac12[T_D^\epsilon,b(E_a)] +12b(Ea)+\frac12b(E_a) −12TDϵ-\frac12T_D^\epsilon {D}\{D\}
12[b(Ea),b(FD)]\frac12[b(E_a),b(F_D)] +12b(FD)+\frac12b(F_D) −12b(Ea)-\frac12b(E_a) {D}\{D\}

The two values a=0,1a=0,1 are both present. Consequently b(LDϵ)b(L_D^\epsilon) cancels, each b(Ea)b(E_a) cancels, and

+TDϵ−12TDϵ−12TDϵ=0.+T_D^\epsilon-\frac12T_D^\epsilon-\frac12T_D^\epsilon=0.

This is strict in the undecorated incidence complex. In PC, the last two terms land in the already established DD-facet occurrence summand and carry

cD(X)⊗hD⊗or⁡(ND).c_D(X)\otimes h_D\otimes\operatorname{or}(N_D).

The first TDϵT_D^\epsilon term is the Cousin lower term of the oppositely oriented entry edge. It lands in that same summand only after applying ϵDentry\epsilon_D^{\rm entry}. Thus the displayed three-term cancellation is precisely the unproved occurrence-decorated square; no other codimension-one term is missing from the saturated leg.

For g∈D6g\in D_6, the finite incidence chain obeys

gγ~Dϵ=γ~gDgϵ.g\widetilde\gamma_D^\epsilon = \widetilde\gamma_{gD}^{g\epsilon}.

A one-step rotation has gϵ=−ϵg\epsilon=-\epsilon and cycles the three channels. After choosing ordered normal lines, the loaded residue transforms by the normal-orientation character χN(g)\chi_N(g):

g[rDϵ]=χN(g)[rgDgϵ].g[r_D^\epsilon] = \chi_N(g)[r_{gD}^{g\epsilon}].

There is no additional deck sign in the incidence chain. The only residual sign is χN(g)\chi_N(g); assigning it a numerical value without fixing the ordered normal convention would be spurious.

What is nevertheless fixed

Let

η6ϵ,PC\eta_6^{\epsilon,{\rm PC}}

denote any PC realization of the saturated tripod extending the established codimension-one terms. Since the two QTDS presentations have identical physical residue on every channel,

Res⁡DPCdPCη6ϵ,PC=0.\operatorname{Res}^{\rm PC}_D d_{\rm PC}\eta_6^{\epsilon,{\rm PC}}=0.

Therefore

rDϵ:=Res⁡DPCη6ϵ,PCr_D^\epsilon := \operatorname{Res}^{\rm PC}_D \eta_6^{\epsilon,{\rm PC}}

is closed whenever ϵDentry\epsilon_D^{\rm entry} makes residue a chain map.

Entry 77 identifies the induced maximally factorized boundary object with the primitive line

J4⊠J4=knr⟨g4⊠g4⟩.\mathcal J_4\boxtimes\mathcal J_4 = \mathbf k_{\rm nr} \langle g_4\boxtimes g_4\rangle.

Hence there is a scalar

[rDϵ]=λDϵ[g4⊠g4].\boxed{ [r_D^\epsilon] = \lambda_D^\epsilon [g_4\boxtimes g_4]. }

One-step rotation sends DD to the next channel and exchanges the two parity sheets. Reflection fixes the symmetric saturated tail. Thus the six numbers λDϵ\lambda_D^\epsilon belong to one D6D_6-orbit, with only the normal-orientation character changing signs. Computing one representative determines all six.

Boundary, deck covariance, and the local Pochhammer identity do not determine its value. If a closed lift with nonzero primitive boundary residue is available, the replacement

η6ϵ,PC⟼η6ϵ,PC+κD,dPCκD=0,\eta_6^{\epsilon,{\rm PC}} \longmapsto \eta_6^{\epsilon,{\rm PC}}+\kappa_D, \qquad d_{\rm PC}\kappa_D=0,

changes λDϵ\lambda_D^\epsilon while preserving the endpoint boundary. The established axioms do not exclude such a lift and do not provide a period that fixes its coefficient. Scalar provenance must select the value through ϵDentry\epsilon_D^{\rm entry}.

Strict zero versus null-homotopy

Because

ΛDϵ−jDϵ=∂(12(τ0+τ1)),\Lambda_D^\epsilon-j_D^\epsilon = \partial\left(\frac12(\tau_0+\tau_1)\right),

changing between the radial and saturated representatives adds an explicit boundary. A literal chain equality

rDϵ=0r_D^\epsilon=0

is therefore not invariant under the allowed filtered chain-homotopy freedom.

The correct condition is

[rDϵ]=0,\boxed{ [r_D^\epsilon]=0, }

or, with a chosen representative, an explicit homotopy

rDϵ=dPCsDϵ.r_D^\epsilon=d_{\rm PC}s_D^\epsilon.

If λDϵ=0\lambda_D^\epsilon=0, the residue is null-homotopic and the six-point contact primitive belongs to the derived residue-free fiber. If it is nonzero, the primitive has a genuine lower factorized obstruction. A point-set strict zero can be imposed only after choosing the null-homotopy; it is not primary data.

Consequence for eight points

The formal pole-grade primitive remains

H8PC=∑DGDPC(η6PC)+HctPC.H_8^{\rm PC} = \sum_D G_D^{\rm PC} (\eta_6^{\rm PC}) +H_{\rm ct}^{\rm PC}.

Its coefficient boundary is exactly

∑Q(qQ+−qQ−)\sum_Q(q_Q^+-q_Q^-)

because entry 23 exhausts the full symbol by GG, RR, and KK. The marked KK part is closed by entry 83. The RR part is factorization-natural in the derived PC category if and only if

λDϵ=0.\lambda_D^\epsilon=0.

There is still no extra unmarked coefficient remainder. The remaining obstruction is the single six-point entry-counit scalar and, separately, the stronger global problem of gluing local quadrangulation half-lines with Jordan higher coherence.

Exact finite content

The finite carrier identities are certified by

research/nima/check_six_point_subdivision_pc.rs

with SHA-256

46021191c34034bf4cd64f5f80e6fe9f0fb39316f86b263fdfeaae9785a310d4

The checker proves the saturated paths, their D6D_6 covariance, and the explicit rational and integral two-chain fillers. It deliberately does not assign a value to ϵDentry\epsilon_D^{\rm entry} or λDϵ\lambda_D^\epsilon.

Decision

Reject:

The established PC map proves that the six-point tripod residue is strictly zero.

Also reject:

Nonzero physical-facet support by itself proves a nonzero residue class.

Promote:

The invariant six-point obstruction is one scalar multiplying the primitive K4×K4K_4\times K_4 boundary line. Strict zero is representative dependent; null-homotopy is the correct condition.

Retain as the next bounded experiment:

Construct ϵDentry\epsilon_D^{\rm entry} from the occurrence-resolved scalar Laurent grade for one center-to-channel edge and pair its residue with the dual g4∨⊠g4∨g_4^\vee\boxtimes g_4^\vee. This computes λDϵ\lambda_D^\epsilon. Rotation and reflection then determine every channel and sheet.

Internal dependencies

View source on GitHub