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Completion independence with an entangled reference

Statement

Under the code and noise hypotheses of support-normalized transpose recovery and completion, use its completed map T and uncompleted map T0, and let V:Cd→HP be an isometry onto the nonzero code. For every finite-dimensional complex inner-product reference space K and every operator W∈L(K⊗Cd), one has

(id⁡K⊗(TNAd⁡V))(W)=(id⁡K⊗(T0NAd⁡V))(W).

Here L(H) denotes the complex-linear endomorphisms of H, Ad⁡V(X)=VXV†, composition is read from right to left, and id⁡K⊗Φ is the linear amplification on operator spaces with the reference factor first, characterized by A⊗B↦A⊗Φ(B). For K=0 it is the unique map between zero operator spaces.

Facts & Assumptions

Given: The finite-dimensional spaces, code, noise, recovery maps and encoding in the Statement.

Goal: Prove equality of the reference-first amplifications on every operator W.

[F1]

The completed and uncompleted transpose maps agree after noise on every code-supported operator X=PXP, not just on states. Support-normalized transpose recovery and completion

[F2]

The encoding is Ad⁡V(X)=VXV†, with V†V=I and code projector P=VV†. The channel and recovery maps are complex-linear. Code restriction and decoded channel types Support-normalized transpose recovery and completion

[F3]

For finite-dimensional complex inner-product spaces with ordered orthonormal bases, the products of their operator matrix units form a basis of the full endomorphism space of their tensor product, including empty dimensions. Tensor products of operator matrix units form a basis

[F4]

Ordered tensor registers have their ordered product bases and product inner products; exchanging two factors is the linear map exchanging their product basis vectors, with inverse the reverse exchange. A zero-dimensional factor gives the zero tensor space. Ordered tensor registers, their inner product, and wire permutations

[F5]

For a complex-linear map Φ:L(H)→L(G) and R=Cr, r≥1, the ancilla-last block map Φ(r):L(H⊗R)→L(G⊗R) is well-defined and linear, and sends the block family [Xij] to [Φ(Xij)]. Finite ancilla amplification is a well-defined block map

[F6]

Every finite-dimensional complex inner-product space admits an orthonormal basis, with the empty basis in dimension zero. Every finite-dimensional real or complex inner product space has an orthonormal basis

Proof

Given: The spaces, maps and operators in the Statement, and the conventions in [F1]–[F6].

Goal: Establish the well-defined reference-first product action and the asserted equality on all W.

Proof technique: direct.

1.1F1F2algebra

For every X∈L(Cd), P(VXV†)P=VXV†, since PV=V and V†P=V† follow from P=VV† and V†V=I. Thus [F1] gives (TNAd⁡V)(X)=(T0NAd⁡V)(X). Both maps are complex-linear.

1.2F4F6choose

If K=0, the input and output tensor spaces, and hence their endomorphism spaces, are zero, so their unique linear maps coincide. Otherwise put r=dim⁡K≥1, choose an ordered orthonormal basis (ki)i<r of K, and let (ei)i<r be the standard basis of R=Cr. For each of the spaces H=Cd and G=HP, choose an ordered orthonormal basis as well.

2.1F4F5step 1.2construct

For a complex-linear Φ:L(H)→L(G), define JH:K⊗H→H⊗R by JH(ki⊗x)=x⊗ei, and define JG in the same way. These maps send product bases bijectively to product bases and preserve the product inner products; their inverses send x⊗ei to ki⊗x. The block-map supplier therefore defines a well-defined linear map ΨΦ(W)=JG−1Φ(r)(JHWJH−1)JG on the full operator space.

3.1F3F5step 2.1algebra

Write Euvki=δviku for the reference matrix units. For any B∈L(H), direct evaluation on x⊗ei shows that JH(Euv⊗B)JH−1 has block B at (u,v) and zero at every other block. By [F5], its image has block Φ(B) at (u,v) and all other blocks zero. Thus ΨΦ(Euv⊗B)=Euv⊗Φ(B). Expanding an arbitrary reference operator A in its matrix entries gives ΨΦ(A⊗B)=A⊗Φ(B). By [F3], this product action uniquely determines a linear map on the full operator space. Consequently the construction is independent of the chosen bases and is precisely the reference-first amplification id⁡K⊗Φ.

4.1F3step 1.1step 1.2step 3.1∎

Expand W in the basis Euv⊗Ljk from [F3], where Ljk are the logical operator matrix units. By step 1.1 the two recovered maps agree on every Ljk; by step 3.1 their reference-first amplifications agree on every Euv⊗Ljk. Linearity proves the claimed equality for every W. Together with the zero-dimensional case in step 1.2 this covers every stated reference space. In particular, taking K=Cd includes the maximally entangled projector.

Depends on

Used by · 1

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