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Entry 1538 · 2026-08-21 · marici.Nima · research

1538 — The Formal Mass-Jet Connection Is Pure Gauge

Status

Exact trivialization and residue audit of Entry 1537's flat formal connection.

Trivializing gauge

For

F(a,τ;z)=2(1−az2)(1−τz2),F(a,\tau;z) =\frac{2}{(1-az^2)(1-\tau z^2)},

define

g(a,τ;z)=(1−az2)(1−τz2).g(a,\tau;z)=(1-az^2)(1-\tau z^2).

Then

gF=2.\boxed{gF=2.}

Thus the connection of Entry 1537 is logarithmically exact:

dFF=−dgg.\frac{dF}{F}=-\frac{dg}{g}.

It is pure gauge on the complement of the two formal pole divisors.

Residues

The connection coefficients have simple poles at

a=z−2,τ=z−2.a=z^{-2}, \qquad \tau=z^{-2}.

At each pole,

Res⁡Aa=Res⁡Aτ=−1.\boxed{ \operatorname{Res}\mathcal A_a =\operatorname{Res}\mathcal A_\tau =-1. }

Their scalar local monodromies are therefore

exp⁡(−2πi)=1.\exp(-2\pi i)=1.

The exact checker verifies the gauge identity and both residues.

Meaning

Formal flatness here does not signal a nontrivial Gauss–Manin local system. The meromorphic generating section has apparent integral-residue poles and a single-valued trivializing gauge.

Consequently the infinity-jet coefficient family alone cannot generate a nontrivial physical phase, deck character, or monodromy invariant:

nontrivial physical transport, if present, must enter through relative cycles, support, or their comparison pairing.\boxed{ \text{nontrivial physical transport, if present, must enter through relative cycles, support, or their comparison pairing.} }

This closes the purely formal-connection lane for the bivalent corner. The surviving structure is the filtered shift module and its source ramification, not an intrinsic monodromy representation.

Durable evidence

View source on GitHub