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Entry 1759 · 2026-08-21 · marici.Nima · research

1759 — The Complete Measurement Packet Splits the Diagonal Rees Mixing

Diagonal pullback

Entry 1758 keeps the calibration normal xx and measurement normal δ\delta separate. Write the regularized curvature polynomial as

xKx=R+xS+x2T,xK_x=R+xS+x^2T,

where R=RparR=R_{\rm par}.

Pull the measurement family to the diagonal

δ=x.\delta=x.

The degenerating fourth scalar then has first coefficient

qx(S)+i(R01−R10).\boxed{ q_x(S)+i(R_{01}-R_{10}). }

Taken alone, this coefficient mixes:

Thus an isolated diagonal scalar does not preserve the bi-Rees separation.

Companion subtraction

The complete labelled packet also contains the nondegenerating real-superposition measurement qxq_x. Applied to the same regularized curvature family, its first calibration coefficient is exactly

qx(S).q_x(S).

Therefore the source-labelled difference is

[qdiagonal]x1−[qx(xKx)]x1=i(R01−R10).\boxed{ \bigl[q_{\rm diagonal}\bigr]_{x^1} -\bigl[q_x(xK_x)\bigr]_{x^1} =i(R_{01}-R_{10}). }

This is precisely the missing residue direction of Entry 1758.

Narrow result

Diagonal specialization mixes support and readout filtrations, but the complete labelled scalar packet carries its own canonical finite-part subtraction. Consequently no filtered extension ambiguity remains after retaining all source measurements.

The distinction is sharp:

Durable artifacts

Next falsifier

Delete the companion real-superposition measurement by a physical symmetry or support restriction. Test whether another source effect supplies the same finite-part subtraction; if none does, the diagonal packet should retain a genuine rank-one filtered extension.

View source on GitHub