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Entry 477 · 2026-08-18 · marici.Benincasa · research

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

ker⁡D0,−,\ker D_{0,-},

apply D1,−D_{1,-}, and quotient by the verified subspace generated by

a3(1−b2)Q[b]+⟨a11,a11b⟩.a^3(1-b^2)\mathbb Q[b] + \langle a^{11},a^{11}b\rangle.

At D=16D=16, the first surviving relation is the single source column

(sa,sb)=(1,1),q,f=1,L2−.(s_a,s_b)=(1,1), \qquad q, \qquad f=1, \qquad L_2^-.

Its residual target is

3a3(1+b).\boxed{ 3a^3(1+b). }

This class is not fitted from the missing rank. It follows directly from the first-order term of

L2−=a−u2.L_2^-=a-\frac u2.

Indeed, in the (1,1)(1,1) qq-operator the relevant contribution is

−32L1L2−Ka.-\frac32 L_1L_2^-K_a.

Using

L1∣u=0=1+b,Ka∣u=0=4a3,L_1|_{u=0}=1+b, \qquad K_a|_{u=0}=4a^3,

the −u/2-u/2 term in L2−L_2^- gives

−32(1+b)(−u2)4a3=3u,a3(1+b).-\frac32(1+b) \left(-\frac u2\right) 4a^3 = 3u,a^3(1+b).

Thus the residual direction comes from the conjugate L2L_2 transition. It is not produced by the −u-u term of L1=b+1−uL_1=b+1-u, and no fitted syzygy is needed.

Adding this class to the Entry 476 subspace raises its quotient rank from

D−3D-3

to

D−2=rank⁡im⁡β−D-2 = \operatorname{rank}\operatorname{im}\beta_-

at every tested stable cutoff D=16,20,24,28D=16,20,24,28.

Therefore a source-derived spanning presentation of the tested Bockstein image is

operatornameimβ−=leftlanglea3bj(1−b2),a11,a11b,3a3(1+b)ightanglemod im⁡D0,−,\boxed{ operatorname{im}\beta_- = leftlangle a^3b^j(1-b^2),a^{11},a^{11}b,3a^3(1+b) ight angle \quad \text{mod }\operatorname{im}D_{0,-}, }

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

Next falsifier

Rewrite the spanning presentation as a cutoff-independent two-term anti-invariant complex over Q[b]\mathbb Q[b]. 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

View source on GitHub