4078 — The Finite-Field Barcode Does Not Determine Its Optical Readout
Status
Established as an exact hostile test for the source-labelled interaction-net barcode packet of Entry 4076.
Question
Does the finite-field barcode packet over , by itself, determine a lift-independent normalized optical analysis row?
Frozen row
Take the first source-labelled first-death analysis row from Entry 4076. It has twenty nonzero coordinates.
Choose its balanced integer lift , with every residue represented in the interval centered at zero.
Choose a second integer lift by adding to one nonzero coordinate of .
Then
and both lifts have identical labelled support.
Exact hostile witness
The two lifts are not projectively proportional. Their normalized rank-one projectors differ by exact squared Frobenius distance
An explicit integer input , supported on the first two labelled coordinates, satisfies
while
Thus the same finite-field barcode row admits two characteristic-zero lifts for which one normalized optical analyzer reports a dark input and the other reports a nonzero response.
Narrow theorem
The finite-field source-labelled barcode packet alone does not determine a characteristic-zero projective analysis row, normalized projector, or optical response.
Finite-field canonicity and chart covariance therefore do not imply lift-independent operational compilation.
What this does not show
This does not prove that no canonical physical lift exists.
It proves that such a lift cannot be inferred from the finite-field packet alone. It must be supplied by additional source authority, for example:
- a characteristic-zero source reduction;
- an integral lattice;
- a polarization;
- a normalized period pairing;
- a physical instrument convention independently derived from the source.
Consequence
The correct architecture is
The second term is genuine data, not harmless presentation.
Next falsifier
Derive one characteristic-zero lift directly from the frozen source relations and compare it with any independently derived integral or period-normalized lift.
Agreement up to the admitted physical gauge would establish operational canonicity. Disagreement would identify the missing normalization datum.