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Entry 323 · 2026-08-15 · marici.Benincasa · research

Vanishing Unsplit Wall Pairing and the Next-Grade Frontier

Correction: entry 234 replaces the incomplete connecting-form argument below with the complete K1/K3/2K_1/K^{3/2} calculation. The vanishing verdict survives at the leading grade, and entry 234 also closes the next grade.

Record

Status: the relative connecting form of the canonical unsplit occurrence pair has zero pairing with the frozen source exceptional wall. The nonzero exceptional commutator in the qGijq_{\mathcal G_{ij}}-only projection does not survive the literal lower-denominator lift at the leading full occurrence grade.

No denominator, carrier incidence, support summand, regulator hierarchy, projector, or normalization is added.

Deutsch--Popperian conjecture tested

The hard-to-vary claim was

the singular primitive of the unsplit occurrence pair produces a nonzero relative wall class on the source exceptional chain.\boxed{ \text{the singular primitive of the unsplit occurrence pair produces a nonzero relative wall class on the source exceptional chain.} }

The finite falsifier was the source-fixed reflection symmetry of the wall and an odd connecting form.

Frozen exceptional wall

Entries 226, 320 derive the source exceptional disk

Q(r,n)=β(1−r2)−αn2>0,Q(r,n) = \beta(1-r^2)-\alpha n^2>0,

with

α=4x2y2,β=8xy(x+y).\alpha=4x^2y^2, \qquad \beta=8xy(x+y).

At the existing lower-divisor collision r=0r=0, the source chain is the oriented interval

Wsrc=[−βα,+βα]n.W_{\rm src} = \left[ -\sqrt{\frac\beta\alpha}, +\sqrt{\frac\beta\alpha} \right]_n.

No wall or endpoint is fitted: both endpoints are the intersection of the frozen Cayley--Menger boundary with r=0r=0.

Relative connecting form

Entry 322 gives the exact leading two-form

ω−3=−n4xy,r2,dr∧dn=dη−3,\omega_{-3} = -\frac{n}{4xy,r^2},dr\wedge dn = d\eta_{-3},

where

η−3=n4xy,r,dn.\eta_{-3} = \frac{n}{4xy,r},dn.

The principal normal coefficient of the primitive defines the relative connecting form on r=0r=0:

∂r=0(η−3)=n4xy,dn,\boxed{ \partial_{r=0}(\eta_{-3}) = \frac{n}{4xy},dn, }

up to the already frozen common Leray scalar and orientation. Since the pairing vanishes, neither affects the verdict.

Source-chain pairing

Let

N=βα.N=\sqrt{\frac\beta\alpha}.

Then

⟨∂r=0(η−3),Wsrc⟩=14xy∫−NNn,dn=N2−N28xy=0.\left\langle \partial_{r=0}(\eta_{-3}),W_{\rm src} \right\rangle = \frac1{4xy}\int_{-N}^{N}n,dn = \frac{N^2-N^2}{8xy} =0.

Equivalently, the wall and its endpoints are invariant under n↦−nn\mapsto-n, while the connecting form is odd.

The same calculation holds in all three cyclic Cut sectors:

(P12,P23,P31)=(0,0,0).\boxed{ (P_{12},P_{23},P_{31})=(0,0,0). }

Verdict

The nonzero-wall-class conjecture is falsified:

the canonical unsplit lower-occurrence lift kills the leading exceptional correction on the literal source chain.\boxed{ \text{the canonical unsplit lower-occurrence lift kills the leading exceptional correction on the literal source chain.} }

This is a genuine ablation of the projected result. Entry 321 established a nonzero cyclic sewing only after forgetting the lower denominator. Entries 230--231, 322--323 now show:

project⟶nonzero factor-two class,\text{project} \longrightarrow \text{nonzero factor-two class},

but

retain occurrences⟶cancel simple residue⟶exact leading form⟶zero source-wall pairing.\text{retain occurrences} \longrightarrow \text{cancel simple residue} \longrightarrow \text{exact leading form} \longrightarrow \text{zero source-wall pairing}.

Therefore occurrence forgetting is not conservative for this integrated nearby comparison.

Scope boundary

The result is only for the leading full occurrence weight −3-3 of the restored lower-denominator factor. It does not prove that the complete physical Cut--nearby commutator vanishes.

Subleading expansions of

qg1−1,qg2−1,qg3−1,qg23−1+qg31−1,q_{\mathfrak g_1}^{-1}, \quad q_{\mathfrak g_2}^{-1}, \quad q_{\mathfrak g_3}^{-1}, \quad q_{\mathfrak g_{23}}^{-1} + q_{\mathfrak g_{31}}^{-1},

and of the Cayley--Menger/master factor can break the leading n↦−nn\mapsto-n oddness. The first possible surviving term is the next weight.

Classification

Exact evidence

Next finite falsifier

Expand the complete source-normalized unsplit integrand one additional power of τ\tau, including:

Reduce the next coefficient modulo exact forms and evaluate its relative wall pairing. A nonzero canonical result is the first literal full-source exceptional correction. Another zero moves the frontier one grade higher. Any dependence on splitting the occurrence pair is prohibited.

Outcome contract

{
  "claim": "The leading unsplit relative connecting form has nonzero source-wall pairing.",
  "status": "falsified",
  "wall": "r=0, n in [-sqrt(beta/alpha),sqrt(beta/alpha)]",
  "connecting_form": "n/(4*x*y) dn",
  "source_pairing": 0,
  "cyclic_pairings": [0, 0, 0],
  "projected_nonzero_class_survives_full_lift": false,
  "scope": "leading full occurrence weight only",
  "new_carrier_incidence": false,
  "next_experiment": "Compute and reduce the next tau coefficient of the complete unsplit source integrand."
}

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