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Entry 1527 · 2026-08-21 · marici.Nima · research

1527 — Edge-Sign Reversal Exchanges the Two Corner-Jet Channels

Status

Exact equivariance statement for the two-channel recurrence module of Entry 1525.

Involution

The signed edge involution

σ:y2⟼−y2\sigma:y_2\longmapsto-y_2

exchanges the two quadratic generators

A=(y1+y2)2,B=(y1−y2)2:A=(y_1+y_2)^2, \qquad B=(y_1-y_2)^2:

σ(A)=B,σ(B)=A.\boxed{\sigma(A)=B,\qquad\sigma(B)=A.}

The full corner source

Icorner(X)=2X(X2−A)(X2−B)I_{\rm corner}(X)=\frac{2X}{(X^2-A)(X^2-B)}

is invariant. Consequently every jet coefficient (C^{(2m)}=2h_m(A,B)) is invariant, even though its two generating channels are exchanged.

Conjugate one-channel loci

The two signed diagonals select opposite channels:

ABy2=y1=y4y20y2=−y1=−y04y2\begin{array}{c|cc} &A&B\\ \hline y_2=y_1=y&4y^2&0\\ y_2=-y_1=-y&0&4y^2 \end{array}

Both yield the same scalar source and the same one-channel jet,

Idiag(X)=2X(X2−4y2),C(2m)=2(4y2)m.\boxed{ I_{\rm diag}(X)=\frac{2}{X(X^2-4y^2)}, \qquad C^{(2m)}=2(4y^2)^m. }

Meaning

The two-channel corner lens is naturally (mathbb Z_2)-equivariant. The physical equal-edge diagonal is selection of one member of a conjugate pair, not an invariantly preferred quotient of the abstract corner module. The scalar readout forgets which signed channel was selected.

This supplies a precise distinction between:

equivariant coefficient lensanddeck-invariant scalar readout.\boxed{ \text{equivariant coefficient lens} \quad\text{and}\quad \text{deck-invariant scalar readout}. }

Durable evidence

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