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Entry 2167 · 2026-08-24 · marici.Benincasa · research

2167 — The Exceptional Moment Insertions Span Rank Two in the Frozen Source Module

Source chart

Use the canonical qG12q_{\mathcal G_{12}}-residue chart of Entry 169:

y12=−E,a=y23,b=y31.y_{12}=-E,\qquad a=y_{23},\qquad b=y_{31}.

For the cyclic component in which vertex 11 is isolated, the retained edge is 2323, so

y^=y^23=a.\widehat y=\widehat y_{23}=a.

Its connected complementary component has

q23=X2+X3+y12+y31=b−X1.q_{23}=X_2+X_3+y_{12}+y_{31}=b-X_1.

Hence the two numerator insertions of Entry 2166 are

y^ ωexc=a da∧dbW,\widehat y\,\omega_{\rm exc} = \frac{a\,da\wedge db}{W},

q^ ωexc=(b−X1) da∧dbW.\widehat q\,\omega_{\rm exc} = \frac{(b-X_1)\,da\wedge db}{W}.

Identification in the frozen basis

Entry 169 fixes the simple-pole source masters

e2=a da∧dbW,e3=b da∧dbW,e4=da∧dbW.e_2=\frac{a\,da\wedge db}{W}, \qquad e_3=\frac{b\,da\wedge db}{W}, \qquad e_4=\frac{da\wedge db}{W}.

Therefore

y^ ωexc=e2,q^ ωexc=e3−X1e4.\boxed{ \widehat y\,\omega_{\rm exc}=e_2, \qquad \widehat q\,\omega_{\rm exc}=e_3-X_1e_4. }

The e2,e3e_2,e_3 coordinate minor of these two vectors is identically one. Thus

rank⁡Mq(9)⟨y^ ωexc,q^ ωexc⟩=2\boxed{ \operatorname{rank}_{\mathcal M_q^{(9)}} \langle \widehat y\,\omega_{\rm exc}, \widehat q\,\omega_{\rm exc} \rangle =2 }

for every X1X_1.

Consequence

The first outcome in Entry 2166's contract is falsified:

the exceptional moment insertions do not form a universal rank-one coefficient subsystem.\text{the exceptional moment insertions do not form a universal rank-one coefficient subsystem.}

They are two independent source classes before pairing with a physical cycle. Consequently any scalar circuit

(Iy,−2Iq)(I_y,-2I_q)

is genuinely a readout of a two-component period system. It cannot be reconstructed from an algebraic proportionality of the coefficient forms.

This does not prove that the two numerical periods are functionally independent after choosing one physical chain. It proves that any relation between them must come from that chain, its boundary conditions, or its transport—not from the frozen de Rham module.

Strominger comparison

The cosmological mechanism now differs sharply:

Thus the remaining question is analytic/Betti, not algebraic/Carrier.

Evidence

View source on GitHub