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Support-normalized transpose recovery and completion

Statement

Let HP,HO be finite-dimensional complex inner-product spaces, let P be the orthogonal projector onto a nonzero code subspace of HP, and let N:L(HP)→L(HO) be a quantum channel with finite Kraus representation N(X)=∑aEaXEa†. Put A=N(P), let S be the orthogonal projector onto supp⁡A=(ker⁡A)⊥, and let A−1/2 be the inverse square root on this support and zero on ker⁡A. Define Ra=PEa†A−1/2 and T0(Y)=∑aRaYRa†.

The map T0 is completely positive, has output supported on the code, and preserves trace for every Y supported on supp⁡A, meaning Y=SYS. For any code state σ—a positive semidefinite operator of trace one with PσP=σ—the map T(Y)=T0(Y)+tr⁡((I−S)Y)σ is a quantum channel with code-supported output. For every X=PXP, the output N(X) is supported on supp⁡A; consequently T(N(X))=T0(N(X)). In particular, completion does not change any recovered code-state output or the value of any function of that output with all other arguments fixed. Explicitly, let ρ be any code state and let τ be any density operator on HP, meaning a positive semidefinite operator of trace one. With the root-fidelity convention F(B,C)=∥BC∥1 for density operators B,C on the same space, where ∥⋅∥1 denotes the trace norm, one has F(τ,T(N(ρ)))=F(τ,T0(N(ρ))). The same equality holds for squared fidelity F2.

Facts & Assumptions

Given: The finite-dimensional spaces, nonzero code projector, channel, Kraus family and code state in the Statement.

Goal: Establish the support normalization, the completed channel, and equality on outputs of code-supported inputs.

[F1]

A quantum channel is linear, completely positive and trace-preserving; a code-supported physical recovery has outputs Z satisfying PZP=Z. Code restriction and decoded channel types

[F2]

For positive semidefinite A, the support inverse square root is zero on the kernel and satisfies A−1/2AA−1/2=S. Finite support square roots and generalized inverses

[F3]

The given Kraus representation means N(X)=∑aEaXEa† for every input operator. Finite Kraus representation

[F4]

For compatible finite matrices, tr⁡(BC)=tr⁡(CB), including rectangular products. For A∈ M_m× n(F) and B∈ M_n× m(F), tr(AB)=tr(BA)

[F5]

For density operators B,C on the same nonzero finite-dimensional complex inner-product space, root fidelity is F(B,C)=∥BC∥1, where ∥⋅∥1 is the trace norm; squared fidelity is F(B,C)2. Fidelity

Proof

technique · direct

Given: The finite-dimensional spaces, nonzero code projector, channel, Kraus family and code state in the Statement.

Goal: Establish the support normalization, the completed channel, and equality on outputs of code-supported inputs.

Proof technique: direct.

1.1givenF2F3F4

Each EaPEa† is positive semidefinite, since its quadratic form at y is the squared norm of PEa†y. Thus A=∑aEaPEa† is positive semidefinite. By [F2], ∑aRa†Ra=A−1/2(∑aEaPEa†)A−1/2=S. Each Ra has range in the code, so PT0(Y)P=T0(Y). Conjugation by any operator remains positive after tensoring with a finite ancilla, and finite sums preserve positivity; hence T0 is completely positive. By [F4], tr⁡T0(Y)=tr⁡(SY), which equals tr⁡Y when Y=SYS.

2.1givenF1F2F4step 1.1

Write Q=I−S. Choose an orthonormal basis (wj) of the range of Q and a spectral decomposition σ=∑ipi∣ui⟩⟨ui∣, where pi≥0, ∑ipi=1, and the vectors with nonzero weights lie in the code. The operators Cij=pi∣ui⟩⟨wj∣ satisfy ∑i,jCijYCij†=tr⁡(QY)σ and ∑i,jCij†Cij=Q. Therefore the completion term is completely positive and code-supported. Together with step 1.1, it makes T completely positive and code-supported; its trace is tr⁡(SY)+tr⁡(QY)=tr⁡Y. Thus T is a channel by [F1].

3.1givenF2F3step 1.1step 2.1

If y∈ker⁡A, then 0=⟨Ay,y⟩=∑a∥PEa†y∥2. Every summand is nonnegative, so PEa†y=0 for every a. Taking adjoints gives QEaP=0 and PEa†Q=0. Hence, for X=PXP, both QN(X)=0 and N(X)Q=0; equivalently N(X)=SN(X)S. Its completion term therefore vanishes.

4.1givenF1F5step 2.1step 3.1∎

For a code state ρ, the operator Z=T(N(ρ)) is positive semidefinite and has trace one because N and T are channels. By step 3.1 it equals T0(N(ρ)), which is therefore also a density operator. For any density operator τ on HP, both sides of the asserted root-fidelity identity are consequently defined by [F5] and equal F(τ,Z). Squaring gives the squared-fidelity identity. More generally, substitution of the equal recovered operators into any function defined at their common value, with all other arguments fixed, gives equal values.

Depends on

Used by · 7

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