The Residual Odd Bockstein Direction Comes from the Conjugate L2 Transition
Record
Status: exact-sector provenance of the one-dimensional residual left by Entry 476.
Retain source labels while reducing the deck-orbit-completed anti-invariant Bockstein. Compute explicit relations in
apply , and quotient by the verified subspace generated by
At , the first surviving relation is the single source column
Its residual target is
This class is not fitted from the missing rank. It follows directly from the first-order term of
Indeed, in the -operator the relevant contribution is
Using
the term in gives
Thus the residual direction comes from the conjugate transition. It is not produced by the term of , and no fitted syzygy is needed.
Adding this class to the Entry 476 subspace raises its quotient rank from
to
at every tested stable cutoff .
Therefore a source-derived spanning presentation of the tested Bockstein image is
with the degree ranges imposed by the filtration. This is a spanning presentation modulo the frozen image; relations among the displayed generators remain part of the quotient.
Classification
- extensive component: source deformation factor ;
- resonance orbit: contained in the Bockstein image;
- residual one-dimensional component: conjugate transition;
- -deformation attribution: refuted for the residual;
- new carrier datum: none.
Next falsifier
Rewrite the spanning presentation as a cutoff-independent two-term anti-invariant complex over . Determine its relations and test whether the physical relative-support functor removes the extensive tail while retaining exactly the reduced odd matrix-factorization line. No tail-removal operation may be introduced merely to force that outcome.
Evidence
- research/benincasa/marici-gm/src/bin/soft_axis_orbit_completed_rank.rs;
- Entries 471 and 473--476.