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Entry 1755 · 2026-08-21 · marici.Nima · research

1755 — Two Measurement Normals Recover Rank-Two Tomography without Excess

Simultaneous rank loss

Let one labelled rank-one effect vary as

∣vε,η⟩=∣0⟩+(ε+iη)∣1⟩.|v_{\varepsilon,\eta}\rangle =|0\rangle+(\varepsilon+i\eta)|1\rangle.

At (ε,η)=(0,0)(\varepsilon,\eta)=(0,0), it coincides with the ∣0⟩|0\rangle effect. Together with the independent ∣1⟩|1\rangle effect, the ordinary packet has rank two and retains only h00,h11h_{00},h_{11}.

The exact two-normal expansion is

qε,η=h00+ε(h01+h10)+iη(h01−h10)+(ε2+η2)h11.\boxed{ q_{\varepsilon,\eta} =h_{00} +\varepsilon(h_{01}+h_{10}) +i\eta(h_{01}-h_{10}) +(\varepsilon^2+\eta^2)h_{11}. }

Hence

gr⁡(1,0)q=h01+h10,gr⁡(0,1)q=i(h01−h10).\operatorname{gr}^{(1,0)}q=h_{01}+h_{10}, \qquad \operatorname{gr}^{(0,1)}q=i(h_{01}-h_{10}).

These two labelled first grades recover both off-diagonal entries:

2h01=gr⁡(1,0)q−igr⁡(0,1)q,2h_{01} =\operatorname{gr}^{(1,0)}q -i\operatorname{gr}^{(0,1)}q,

2h10=gr⁡(1,0)q+igr⁡(0,1)q.2h_{10} =\operatorname{gr}^{(1,0)}q +i\operatorname{gr}^{(0,1)}q.

Mixed-grade test

The expansion has no εη\varepsilon\eta term:

gr⁡(1,1)q=0.\boxed{ \operatorname{gr}^{(1,1)}q=0. }

Therefore the two specialization orders commute. The pure second grades both contain the already known h11h_{11}; they introduce no additional tomographic direction.

Narrow result

A codimension-two tomographic rank loss closes under the existing labelled multi-Rees calculus:

rank-two ordinary packet+two independent first grades=complete rank-four readout.\text{rank-two ordinary packet} + \text{two independent first grades} = \text{complete rank-four readout}.

There is no mixed commutator and no excess coefficient class in this tested rank-one measurement family. No new carrier stratum is required.

Durable artifacts

Next falsifier

Replace the scalar measurement parameters by a noncommuting matrix-valued calibration acting on the effect frame. Compute whether the mixed grade is the calibration commutator and classify it as coefficient curvature rather than carrier excess.

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