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Dimensional boundary of a rank-one KL obstruction

Statement

Let HL,HP,HO be finite-dimensional complex inner-product spaces, with inner products linear in the first argument, and let V:HL→HP be an isometry. Write P=VV∗ for the orthogonal projector onto the code V(HL), and suppose dim⁡HL≥2. Let a channel N:L(HP)→L(HO) be exactly correctable on this code and have a finite Kraus representation containing the nonzero operator E:HP→HO given by Ex=⟨x,s⟩f for vectors s∈HP and f∈HO. Then Ps=0.

The dimension hypothesis is essential: in dimension one, exact correctability and the same rank-one form need not imply Ps=0.

Facts & Assumptions

[F1]

The code projector is P=VV∗, and exact correctability means that a decoded recovery channel composed with the noise and encoding is the identity on the logical operator space. Code restriction and decoded channel types

[F2]

A finite Kraus representation has the form N(X)=∑aEaXEa∗ for every input operator X. Finite Kraus representation

[F3]

The adjoint is characterized by ⟨Tx,y⟩=⟨x,T∗y⟩. The adjoint T^*:W→ V is characterised by ⟨ Tv,w⟩_W=⟨ v,T^*w⟩_V

[F4]

Exact correction of a finite-dimensional isometric code for a channel with finite Kraus operators Ea implies PEa∗EbP=CabP for scalars Cab. Exact recovery implies the Knill–Laflamme condition

Proof

Given: The finite-dimensional isometric code, its exact recovery, and a finite Kraus family containing the stated nonzero E.

Goal: Prove Ps=0 and exhibit the stated one-dimensional boundary.

1.1givenF3F4algebra

By [F4], applied to the index of E twice, PE∗EP=cP for a scalar c. By [F3] and the displayed formula for E, for every x∈HP one has PE∗EPx=∥f∥2⟨x,Ps⟩Ps. Thus the image of PE∗EP lies in the span of Ps, which has dimension at most one.

2.1givenstep 1.1algebra

The image of P is the code and has dimension at least two, so cP cannot have image of dimension at most one unless c=0. Hence PE∗EP=0. Evaluating its quadratic form at s gives 0=∥f∥2∥Ps∥4. Since E is nonzero, f≠0, and therefore Ps=0.

3.1F1F2constructalgebra∎

For the boundary, take all three spaces to be C, let V=P=I, and let N be the identity channel with its single Kraus operator E=I. With s=f=1, the stated rank-one formula holds, the identity channel is its own decoder, and Ps=1≠0. This establishes the claimed one-dimensional exception.

Depends on

Used by · 3

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