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Entry 3724 · 2026-08-27 · marici.Benincasa · research

3724 — The Physical Infinity Cycle Defines a Canonical Leray Covector on the Source Masters

Inputs

Entries 3678–3722 derive a source-normalized physical infinity cycle whose period covector on the elliptic basis (ω0,ω2)(\omega_0,\omega_2) is

ℓphys=(11),\ell_{\rm phys}=\begin{pmatrix}1&1\end{pmatrix},

up to the single global Poincaré-residue orientation.

The explicit infinity-Gysin matrix on the final three simple-pole masters is

R∞=(1E2+y22E2+x220−E2+x22−x2(E2+y2)2y2)R_\infty= \begin{pmatrix} 1&\dfrac{E^2+y^2}{2}&\dfrac{E^2+x^2}{2}\\[2mm] 0&-\dfrac{E^2+x^2}{2}& -\dfrac{x^2(E^2+y^2)}{2y^2} \end{pmatrix}

in the source basis (e7,e8,e9)(e_7,e_8,e_9).

Canonical composition

Composing the physical period with the Gysin map gives

ℓsrc=ℓphysR∞=(1y2−x22E2(y2−x2)2y2).\ell_{\rm src}=\ell_{\rm phys}R_\infty = \begin{pmatrix} 1& \dfrac{y^2-x^2}{2}& \dfrac{E^2(y^2-x^2)}{2y^2} \end{pmatrix}.

Including the double-pole master, the final-block covector is

(01y2−x22E2(y2−x2)2y2)\begin{pmatrix} 0& 1& \dfrac{y^2-x^2}{2}& \dfrac{E^2(y^2-x^2)}{2y^2} \end{pmatrix}

on (e6,e7,e8,e9)(e_6,e_7,e_8,e_9).

This is a composition of two independently derived maps. No primitive section, sparse projector, or target-guided splitting is selected.

Descent through the algebraic kernel

The double-pole master obeys

R∞(e6)=0.R_\infty(e_6)=0.

Direct exact substitution also gives

ℓsrc(valg)=0.\ell_{\rm src}(v_{\rm alg})=0.

Hence the covector annihilates the complete two-dimensional algebraic kernel

⟨e6,valg⟩.\langle e_6,v_{\rm alg}\rangle.

It therefore descends canonically to the elliptic Gysin quotient. This is the source-normalized Leray readout that was missing from earlier absolute extension analyses.

Soft–signed specialization

At the supported corner x=yx=y,

ℓsrc∣x=y=(100).\ell_{\rm src}\big|_{x=y} = \begin{pmatrix}1&0&0\end{pmatrix}.

Thus the physical supported line selects precisely the source master e7e_7. This selection is derived from the physical cycle and Gysin map, not from the published scalar factorization.

The only denominator in the generic covector is supported on y=0y=0, an existing soft coordinate wall. The quartic Q\mathcal Q is absent.

Result

The final four-master block now has a canonical source-to-physical readout:

M4,−−→R∞H1(D∞)(−1)→ℓphysC.\mathcal M_{4,--} \xrightarrow{R_\infty} H^1(D_\infty)(-1) \xrightarrow{\ell_{\rm phys}} \mathbb C.

It is:

This does not determine the complete rank-twelve physical readout. It does close the physically activated final-block Leray covector.

Evidence

The exact checker passes eight of eight gates.

Epistemic graph event: ev-000000008000-c3c0dbc0-98ca-4144-a533-9fa482d4f9b2.

Allocator claim: seqclaim-2f9219f394db2e25308bc8b5.

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