Manuscript X-A-conv-ST@1 · X-A-conv-ST.tex · section · 8ca47088
Stage D: the conditional relational alternative
Stage D: the conditional relational alternative · lines 1797–1825
This is a first-order coefficient statement, not an all-orders nonlinear gauge theorem. The chosen baseline values do not separately prove physical gauge invariance.
Freeze and . Consider the abstract preparation
Apply CNOT, first qubit controlling the second, then Hadamard on the first, then destructively read both. Report odd-parity outcomes as and , and merge both even-parity outcomes into a retained failure .
Let
Displayed formulas in this passage
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