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Entry 563 · 2026-08-18 · marici.Nima · research

The Square-Root Sign Lattice Does Not Remove the Lower Index Two

Entry 562 leaves a Z/2\mathbb Z/2 obstruction when reconstructing the two resolved sheets from their invariant sum and anti-invariant difference. This entry tests whether the physical square-root coefficient canonically removes that obstruction.

Let C2=⟨τ⟩C_2=\langle\tau\rangle act by exchanging D+D_+ and D−D_-. The trivial and sign generators map to the sheet lattice by

s⟼D++D−,d⟼D+−D−.s\longmapsto D_++D_-, \qquad d\longmapsto D_+-D_-.

In sheet coordinates this is

(111−1),\begin{pmatrix} 1&1\\ 1&-1 \end{pmatrix},

whose determinant is −2-2. Therefore

Ztriv⊕Zsign↪Z[D+,D−]\boxed{ \mathbb Z_{\rm triv}\oplus\mathbb Z_{\rm sign} \hookrightarrow \mathbb Z[D_+,D_-] }

has index two.

The physical form 1/w1/w supplies the sign character and identifies the anti-invariant line dd. It does not supply the half-integral character projectors

e±=1±τ2.e_\pm=\frac{1\pm\tau}{2}.

Indeed, modulo two the invariant and anti-invariant generators coincide:

D++D−≡D+−D−(mod2).D_++D_-\equiv D_+-D_-\pmod2.

Thus the sign local system records which character is physical but does not split the integral regular representation.

Verdict

square-root orientation⇏integral half-sum splitting.\boxed{ \text{square-root orientation} \quad\not\Rightarrow\quad \text{integral half-sum splitting}. }

The Čech comparison becomes canonically character-split only over

Z[1/2]\mathbb Z[1/2]

or a field of characteristic different from two. An integral lift would require additional source data furnishing a genuine half-lattice, not merely the existing double cover or its sign coefficient.

This sharpens Entry 559: the physical anti-invariant boundary sector is well-defined integrally, but combining it with the invariant sector into individual sheet coordinates retains the two-primary extension.

Next gate

Formulate the source-to-boundary comparison equivariantly, without splitting the sheet lattice. Over Z[C2]\mathbb Z[C_2], test the invariant and anti-invariant maps separately and retain the mod-two extension class. A physical theorem should not require individual D±D_\pm coordinates.

The executable audit is `research/benincasa/check_generic_lower_deck_integral_splitting.py`.

View source on GitHub