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Exact four-level transpose fidelity

PDF p. 8: Eq. (S1.7) and following equivalence

Statement

Assume the postulated four-level model with orthonormal basis ∣0⟩,∣1⟩,∣2⟩,∣3⟩, code C=span⁡{∣0⟩,∣1⟩}, decay rate γ≥0, real splitting Δ, and time t≥0. Let HL=C2 have ordered orthonormal basis ∣0⟩L,∣1⟩L, and encode by the isometry V:HL→C4 with V∣j⟩L=∣j⟩ for j=0,1. Write Nt for the model channel and Tt for any support-completed transpose recovery for the code projector P=VV†. The resulting decoded logical channel is Et(X)=V†Tt(Nt(VXV†))V. Let Ftr(t) be the entanglement fidelity of the resulting logical channel at the maximally mixed logical input I/2.

For γt>0, set pdecay=1−e−γt and χd(t)=γ(eiΔt−e−γt)/[(γ+iΔ)(1−e−γt)]. Then

Ftr(t)=1−pdecay2(1−∣χd(t)∣2)=(γ2+Δ2)sinh⁡(γt)+γ2[cosh⁡(γt)−cos⁡(Δt)](γ2+Δ2)(eγt−1).

At γt=0, the fidelity is 1; the conditional decay coherence is not assigned at zero decay probability. The displayed quotient has the same limiting value 1 as γt→0 along the model parameter domain.

Facts & Assumptions

[F1]

In the postulated model the code and decay spans are orthogonal, and the evolution is the specified finite-dimensional channel with γ≥0, real Δ, and t≥0. Four-level spontaneous-decay model

[F2]

On the code, the exact channel has a no-jump branch of weight e−γt and a decay branch with diagonal weight p=1−e−γt and off-diagonal coefficient c=γ∫0te−γseiΔ(t−s) ds. In particular ∣c∣≤p, and the branch maps into the decay span. Exact four-level Kraus operators

[F3]

For p>0, identifying ∣2⟩,∣3⟩ with the logical basis gives the normalized decay coherence χd=c/p as displayed in the statement; the normalized no-jump output is the input. Conditional decoded state and decay coherence

[F4]

The support-completed transpose recovery uses the inverse square root of the channel output on the code projector on its support, and its completion does not affect outputs of encoded inputs. Transpose (Petz) recovery on a code

[F5]

A qubit coherence map Dλ preserves diagonal matrix entries and multiplies the 01 entry by λ and the 10 entry by its conjugate. For ∣λ∣≤1 its entanglement fidelity at I/2 is (1+Re⁡λ)/2, and fidelity is affine under a weighted sum of channels. Qubit coherence channels and fidelity functionals

[F6]

For a channel with orthogonal flagged branches (1−p)id⁡ and pDχ, its support-normalized transpose recovery produces the logical channel (1−p)id⁡+pD∣χ∣2, including zero-weight branches. Transpose recovery for a flagged coherence channel

[F7]

Matrix entries, adjoints and basis identifications follow the finite orthonormal-basis conventions. Finite operator and ket conventions

[F8]

For an isometric encoding V with code projector P=VV† and a code-supported physical recovery Tt, the decoder is Y↦V†Tt(Y)V, and composing it with Nt∘Ad⁡V gives the logical channel Et in the statement. Code restriction and decoded channel types

Proof

Given: The model, code, parameters and transpose-recovery procedure in the statement.

Goal: Compute the fidelity, prove the two formulas agree, and establish the zero-decay boundary.

1.1givenF1F2F3F5F7F8

Put q=e−γt and p=1−q. By [F1] and [F2], the output restricted to encoded inputs has two orthogonal flags: the code span and the decay span. Identify the code span with HL by V and the decay span by the isometry W∣j⟩L=∣j+2⟩ for j=0,1. The no-jump branch is qid⁡; the decay branch preserves diagonal entries with coefficient p and multiplies the 01 entry by c. Thus, when p>0, the restricted channel is the flagged channel qid⁡⊕pDχ with χ=c/p=χd. The bound in [F2] gives ∣χ∣≤1. These equalities hold on all input matrices by their entries, not merely on a chosen state.

2.1givenF4F6F7F8step 1.1algebra

Let Kk be the model-channel Kraus matrices and put Bk=KkV. The restricted noise Nt∘Ad⁡V has Kraus matrices Bk, and A=Nt(P)=∑kBkBk†. By [F4] and [F8], its decoded support-normalized recovery has Kraus matrices V†PKk†A−1/2=Bk†A−1/2, since V†P=V†. These are exactly the transpose-recovery matrices for the restricted channel with whole input code HL. The completion has no effect on the restricted noise outputs by [F4]. Thus the physical recovery and decoding defining Et agree, under the basis identifications of step 1.1, with the recovered flagged channel in [F6].

3.1F4F5F6F8step 1.1step 2.1algebra

Applying the flagged transpose rule to step 1.1, using the decoded-recovery identification in step 2.1 and the support convention in [F4], gives qid⁡+pD∣χd∣2. The fidelity formula and affinity in [F5] therefore give Ftr=q+p(1+∣χd∣2)/2=1−p(1−∣χd∣2)/2. This proves the first expression when p>0.

4.1F3step 3.1algebra

For p>0, write D=γ2+Δ2>0. Directly taking the modulus in [F3] gives ∣χd∣2=γ2(1+q2−2qcos⁡(Δt))/(Dp2). Substitution into step 3.1 and multiplication of numerator and denominator by eγt yield Ftr=[Dsinh⁡(γt)+γ2(cosh⁡(γt)−cos⁡(Δt))]/[D(eγt−1)], proving the printed quotient and its equivalence to the first expression.

5.1givenF2F6step 1.1step 3.1step 4.1algebra∎

If γt=0, then p=0 and [F2] gives no decay branch; the no-jump branch is the identity on the encoded logical qubit. The zero-weight case of [F6] therefore gives fidelity 1. For p>0, step 1.1 gives 0≤∣χd∣2≤1, so step 3.1 implies 0≤1−Ftr≤p/2. As γt→0, p→0, establishing the stated limit of both formulas without assigning a conditional state to the zero-weight branch.

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