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Long-time four-level transpose plateau

PDF p. 8: Eq. (S1.8)

Statement

Assume the postulated four-level model with code C=span⁡{∣0⟩,∣1⟩}, decay rate γ≥0 and real energy splitting Δ. Encode a logical qubit in the code, apply the model channel for time t≥0, apply its support-completed transpose recovery, and decode. Let Ftr(t) be the entanglement fidelity of the resulting logical channel at the maximally mixed logical input I/2.

If γ>0, then

lim⁡t→∞Ftr(t)=12(1+γ2γ2+Δ2).

At Δ=0 the recovered logical channel is the identity for every t≥0, so recovery is perfect. For fixed γ>0, the plateau tends to 1/2 as ∣Δ∣/γ→∞. In that limit the recovered decay branch approaches complete dephasing in the logical basis: it retains the diagonal entries and removes both off-diagonal entries. This is the model's operational meaning here of fully distinguished decay paths, rather than a claim of a measured environment state.

If γ=0, there is no decay and the recovered logical channel is the identity for all t and all Δ; in particular its long-time fidelity is 1. The positive-rate plateau formula is not applied at γ=0.

Facts & Assumptions

[F1]

The four-level postulate specifies the code, nonnegative decay rate, real splitting and model channel. Four-level spontaneous-decay model

[F2]

Transpose recovery uses the inverse square root on the support of the channel output on the code projector; its completion has no effect on encoded inputs. Entanglement fidelity at I/2 is the overlap of a maximally entangled purification with its output under the logical channel. Transpose (Petz) recovery on a code Entanglement fidelity on a finite logical space

[F3]

For γt>0, put q=e−γt, p=1−q and χ=γ(eiΔt−q)/[(γ+iΔ)p]. The exact fidelity is Ftr=1−p(1−∣χ∣2)/2. At γt=0 it is 1. Exact four-level transpose fidelity

[F4]

The noise restricted to the code has orthogonal no-decay and decay branches of weights q and p. The no-decay branch is the identity under the stated basis identification. For a complex multiplier χ, write Dχ for the entrywise linear map that preserves diagonal entries and multiplies the 01 and 10 entries by χ and χ‾. For ∣χ∣≤1 this map is a qubit channel. The identification of the normalized decay branch with this map and the required bound ∣χ∣≤1 are established below using the Kraus representation and the conditional-state input [F8]. Exact four-level Kraus operators Qubit coherence channels and fidelity functionals

[F5]

For such orthogonal flagged branches the transpose-recovered logical channel is qid⁡+pD∣χ∣2 when p>0; the zero-weight case gives the identity when p=0. Transpose recovery for a flagged coherence channel

[F6]

The real exponential tends to zero at negative infinity, and ∣eiy∣=1 for real y. The exponential tends to +∞ at +∞ and to 0 at -∞ exp(x+iy)=eˣ(cos y+i sin y), |exp(x+iy)|=eˣ, and e^iπ+1=0

[F7]

Matrices, adjoints, outer products and basis identifications use the finite orthonormal-basis conventions. Finite operator and ket conventions

[F8]

The syndrome recovery uses the code projector P and the partial isometry U=∣0⟩⟨2∣+∣1⟩⟨3∣, with branch operations Y↦PYP and Y↦UYU†. For every normalized code vector a∣0⟩+b∣1⟩ and p>0, its normalized recovered decay state has diagonal entries ∣a∣2,∣b∣2 and 01 entry ab‾χ, with χ exactly as in [F3]; the outcome probability p is independent of the vector. Its normalized null output is the input, with probability q. These are conditional-state formulas for this syndrome recovery, used only to identify the noise blocks before applying the transpose rule. Four-level syndrome recovery Conditional decoded state and decay coherence

Proof

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

Goal: Establish the plateau, its two limiting interpretations and the zero-rate boundary.

1.1givenF3F4F7F8algebra

Write N=Nt, put q=e−γt and p=1−q for all model parameters, and use the logical basis ∣0⟩L,∣1⟩L of C2. Define V∣j⟩L=∣j⟩ and W∣j⟩L=∣j+2⟩ for j=0,1. Then P=VV† and U=VW† in [F8]. The Kraus operators cited in [F4] map encoded inputs into separate code and decay blocks: K1V is a scalar of squared modulus q times V, and K2V,K3V have range in the decay span. Thus there are no cross-block terms. For p>0, define the complex-linear map B(X)=p−1W†N(VXV†)W. By [F8] and U=VW†, B(∣ψ⟩⟨ψ∣) has exactly the entries prescribed by Dχ for every unit logical vector ψ. This identifies the map on all matrices: put Ejk=∣j⟩L⟨k∣L, G+=∣+⟩⟨+∣ and Gi=∣+i⟩⟨+i∣, where ∣+⟩=(∣0⟩L+∣1⟩L)/2 and ∣+i⟩=(∣0⟩L+i∣1⟩L)/2. The four pure projectors E00,E11,G+,Gi span the complex matrix space, since S=2G+−E00−E11=E01+E10 and T=2Gi−E00−E11=−iE01+iE10 give E01=(S+iT)/2 and E10=(S−iT)/2. Complex linearity therefore gives B=Dχ and N(VXV†)=qVXV†+pWDχ(X)W† for every logical matrix X. When p=0, the endpoint Kraus operators give N(VXV†)=VXV† without defining χ.

1.2givenF3F6algebra

Suppose γ>0. By [F6], q=e−γt→0 and hence p→1 as t→∞. Since ∣eiΔt∣=1, the triangle inequality gives 1−q≤∣eiΔt−q∣≤1+q. The bounds converge to 1, so directly from the definition in [F3], ∣χ∣2→γ2/(γ2+Δ2). Substitution in [F3] proves the displayed plateau.

2.1givenF4F7F8step 1.1algebra

For p>0, the Kraus representation makes B(G+) positive semidefinite: for every vector w, w†B(G+)w=p−1∑j∣w†W†KjV∣+⟩∣2≥0. By step 1.1 its matrix is 12(1χχ‾1). If r=∣χ∣>0, evaluate its quadratic form at w=(χ/r,−1)T: it equals 1−r, so r≤1. If χ=0, the same bound is immediate. Also q,p are the nonnegative outcome probabilities in [F8], with q+p=1. Thus the flagged transpose rule's parameter hypotheses hold.

3.1givenF2F4F5F7step 1.1step 2.1algebra

To identify the physical transpose recovery with the rule in [F5], put Bj=KjV and A=N(P)=∑jBjBj†. By [F2], the decoded support-normalized recovery has Kraus matrices V†PKj†A−1/2=Bj†A−1/2; these are precisely the transpose matrices for the restricted noise with whole logical input as code. The support completion has no effect after noise on an encoded input. Under the orthogonal identifications V,W, steps 1.1 and 2.1 therefore allow [F5] to give the recovered channel qid⁡+pD∣χ∣2 for p>0. For p=0 it gives the identity, with no conditional decay state.

4.1givenF2F3F4F5step 3.1algebra

If Δ=0 and γt>0, the expression in [F3] gives χ=1. The entrywise definition in [F4] makes D1 the identity, so [F5] gives the identity recovered channel. At γt=0, [F5] gives the same result. Thus every logical input is recovered, and its entanglement fidelity is 1 by [F2].

4.2givenF4F5step 1.2step 3.1algebra

For fixed γ>0, the ratio γ2/(γ2+Δ2)=1/(1+(Δ/γ)2) tends to zero as ∣Δ∣/γ→∞. Step 1.2 therefore gives plateau 1/2. By [F4] and [F5], the recovered decay branch is D∣χ∣2. Taking first t→∞ and then ∣Δ∣/γ→∞ sends its off-diagonal multiplier to zero while leaving its diagonal entries fixed. The limiting channel is therefore complete dephasing. Its two basis inputs remain orthogonal while their coherence is lost, giving the stated operational interpretation.

5.1givenF2F4F5step 3.1algebra∎

If γ=0, then p=0 for every time. The no-decay branch is the identity and the decay branch has zero weight by [F4]; [F5] gives the identity recovered channel. Its fidelity is consequently 1 by [F2]. This establishes the separate zero-rate boundary.

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