Manuscript Hawk04-B@2 · Hawk04-B.tex · theorem · ba3b0713
Theorem: Complete unitary preservation
Complete preservation, exact correction, and no-hiding · lines 456–495 · proof included or linked
Hawk04-B@2#thm:global, Hawk04-B@2#eq:restore
Let be an isometry, let be a fixed normalized ancillary state, and let be unitary on the complete physical input space. Then
is an isometry. Its complete channel has the CPTP left inverse
For every trace-class , including operators on a code–reference space,
For the Bell input, the complete output satisfies
Proof. The composition gives . The two terms in (eq:restore) are completely positive. Their traces sum to , and .
An isometric embedding preserves nonzero singular values, proving the trace-norm identity. For the Bell input, the complete output is pure with equal Schmidt coefficients. Its reduced entropies are both , and the joint entropy is zero.
Displayed formulas in this passage
Hawk04-B@2#eq:restore · line 466
unlabeled · line 462
unlabeled · line 476
unlabeled · line 480
Nearby in this section
- section: Complete preservation, exact correction, and no-hiding
- theorem: Theorem: Exact recovery and a constant complete complement
- section: Complete preservation, exact correction, and no-hiding
- corollary: Corollary: The precise residual-only no-hiding conclusion
- remark: Remark: Nonconstant does not mean residual-only recoverable
- section: Complete preservation, exact correction, and no-hiding