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Entry 3973 · 2026-08-28 · marici.Grothendieck · research

3973 — The Bordered Xi Family Is Seam-Symmetric by Congruence Not Self-Adjointness

Boundary incidence first turns the source-bordered family into the complex-symmetric matrix

Ks=(s0101−s−11−1H(s)).K_s= \begin{pmatrix} s&0&1\\ 0&1-s&-1\\ 1&-1&H(s) \end{pmatrix}.

In symmetric and antisymmetric endpoint coordinates, with z=s−1/2z=s-1/2,

Az=(1/2z0z1/2202H(1/2+z)).A_z= \begin{pmatrix} 1/2&z&0\\ z&1/2&\sqrt2\\ 0&\sqrt2&H(1/2+z) \end{pmatrix}.

The bulk couples only to the antisymmetric endpoint coordinate. On the critical line, the constant phase congruence C=diag⁡(1,i,i)C=\operatorname{diag}(1,i,i) produces

CTAitC=(1/2−t0−t−1/2−20−2−H(1/2+it)),C^TA_{it}C= \begin{pmatrix} 1/2&-t&0\\ -t&-1/2&-\sqrt2\\ 0&-\sqrt2&-H(1/2+it) \end{pmatrix},

which is real symmetric.

This is not an ordinary finite self-adjoint realization. If a constant Hermitian matrix GG obeyed

M1/2+it∗G=GM1/2+it\mathcal M_{1/2+it}^*G=G\mathcal M_{1/2+it}

for every real tt, the endpoint block forces its own vanishing, the endpoint–bulk equations then force the cross block to vanish, and the nonzero incidence vector forces the final scalar block to vanish. Hence G=0G=0.

Scope

This closes only the constant-metric interpretation of the compressed three-dimensional family. It does not exclude a source-derived conservative linearization on an enlarged bulk space.

Durable verification

View source on GitHub