Manuscript Hawk05-B@1 · Hawk05-B.tex · theorem · f2e5d4f5
Theorem: Clean flagged formulas and the complete record
Explicit entropy–recovery separations › The corrected single-excitation calibration · lines 1251–1326 · proof included or linked
Hawk05-B@1#thm:flagged, Hawk05-B@1#eq:flaggederrors, Hawk05-B@1#eq:flaggedentropy, Hawk05-B@1#eq:flagrecorderror, Hawk05-B@1#eq:flagrecordentropy
For ,
Immediate cell readout returns histories consisting of either no emission or an emission time and basis label . For , their probabilities are
Its recovery error and complete-record entropy are
If and , then
If , the increment is zero.
Proof. The channels are orthogonal-block channels
The decoder compressing the occupied block and preparing on vacancy gives the radiation upper bound . On a Bell input, no decoder has overlap greater than , proving optimality. Interchanging occupied probabilities gives the residual recovery error. The exact residual leakage is proved in Appendix app:flag; it is , not residual recovery. The entropy formulas follow from the orthogonal blocks.
Successive local readouts may be commuted past later rotations on other cells for the purpose of computing the complete outcome law. Their probabilities are therefore and .
Preparing on a reported label and on no emission gives decoded channel . Its error is at most . The Bell test gives the same lower bound, irrespective of emission time. The history entropy follows by splitting the no-emission branch and then its label. At the next opportunity only the former no-emission outcome is refined, giving the displayed increment.
Displayed formulas in this passage
Hawk05-B@1#eq:flaggederrors · line 1254
Hawk05-B@1#eq:flaggedentropy · line 1254
Hawk05-B@1#eq:flagrecorderror · line 1277
Hawk05-B@1#eq:flagrecordentropy · line 1277
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