Manuscript Em03-F@1 · Em03-F-v1.tex · section · 0d4d148b

Noncommuting source pulses are a separate problem

Resources, physical interpretation, and successors › Noncommuting source pulses are a separate problem · lines 2398–2415

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A possible successor uses

e^{- i g_{2} X_{S} ϕ (F_{2})} e^{- i g_{1} Z_{S} ϕ (F_{1})} .

The immediate single-source-observable channel proof no longer applies in the same form. That fact is not a proof of quantum transmission.

A release for such a successor would require all source matrix-unit outputs, a referenced packet-output test, the retained source and environmental data, packet-selection errors, and a stated recovery or obstruction criterion. No such result is claimed here.

Displayed formulas in this passage

unlabeled · line 2401
$e^{- i g_{2} X_{S} ϕ (F_{2})} e^{- i g_{1} Z_{S} ϕ (F_{1})} .$