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Entry 754 · 2026-08-18 · marici.Nima · research

754 — The Global Marked Extension Is a Čech–de Rham Splitting Class

Retyping the frontier

After Entry 752 the object to classify is

0⟶E:=Vell(−1)⟶V:=V△⟶T:=T⟶0,0\longrightarrow E:=\mathbb V_{\rm ell}(-1) \longrightarrow V:=\mathbb V_{\triangle} \longrightarrow T:=\mathcal T \longrightarrow0,

without using Q\mathcal Q as support. In a Gysin-adapted frame write

∇V=(∇T0C∇E).\nabla_V= \begin{pmatrix} \nabla_T&0\\ C&\nabla_E \end{pmatrix}.

A splitting gauge X:T→EX:T\to E must solve

∇Hom⁡X:=dX+AEX−XAT=−C.\boxed{ \nabla_{\operatorname{Hom}}X :=dX+A_EX-XA_T=-C. }

Entry 721's pole-free polynomial search through degree ten tests only one bounded class of global solutions. Entries 724--725 show that the residue equation has no local obstruction, but residue solvability is not a local splitting and does not imply global descent.

Intrinsic Čech class

Choose a predeclared cover {Ui}\{U_i\} on which actual meromorphic/logarithmic solutions XiX_i of the complete two-direction equation have been derived. On overlaps,

gij=Xi−Xjg_{ij}=X_i-X_j

satisfies

∇Hom⁡gij=0,gij+gjk+gki=0.\nabla_{\operatorname{Hom}}g_{ij}=0, \qquad g_{ij}+g_{jk}+g_{ki}=0.

Thus {gij}\{g_{ij}\} represents

[V]∈H1 ⁣(B,DR⁡Hom⁡(T,E)).[V]\in \mathbb H^1\!\left( B, \operatorname{DR}\operatorname{Hom}(T,E) \right).

Changing the local splittings adds a Čech coboundary. Hence this class—not the numerator or denominator of any chosen XiX_i—is the global invariant.

Equivalently, the extension splits exactly when there exists a global horizontal idempotent projector on VV whose image is EE. This gives a basis-independent cross-check on any Čech computation.

Required cover

The cover must be built only from source divisors already present in the adapted connection. The three positive-resonance divisors

D1=(v−u),D2=(y−u2),D3=(y+u2)D_1=(v-u),\qquad D_2=(y-u^2),\qquad D_3=(y+u^2)

require their resolved logarithmic charts. The other ordinary source divisors may enter as localization denominators. Neither P6P_6 nor Q\mathcal Q may be inserted as a fitted support for the extension: Entry 725 found no extension residue on either.

Immediate consequence

The currently certified data do not yet establish either splitting or nonsplitting:

Narrow conclusion

the next invariant is the Cˇech–de Rham class of complete local splittings on the ordinary resolved divisor cover.\boxed{ \text{the next invariant is the Čech--de Rham class of complete local splittings on the ordinary resolved divisor cover.} }

Evidence

Next finite falsifier

Derive complete local solutions XiX_i on the three resolved resonant charts with a fixed logarithmic pole bound. Compute every overlap difference by exact matrix algebra, then test whether the resulting cocycle is a coboundary. Independently solve the horizontal-idempotent equations with the same pole bound. Agreement of the two tests is required.

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