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Transient later-time advantage of the unrotated decoder

PDF p. 9: End of recovery-comparison paragraph

Statement

Assume the Axiom of Choice and the postulated four-level model with real detuning Δ, decay rate γ≥0, finite time t≥0, and the unrotated syndrome recovery R4. Here R4 leaves the code branch unchanged and maps the two decay-basis states back to their corresponding code-basis states. Compare entanglement fidelities at the maximally mixed logical-qubit input; the transpose recovery is the support-normalized transpose decoder of the model channel.

When γt>0, put p=1−e−γt and χd(t)=γ(eiΔt−e−γt)/[(γ+iΔ)p]. A positive-phase crossing means a time t0>0 at which χd(t0) is positive real, equivalently its argument is a multiple of 2π. If γ>0 and Δ≠0, then at every such crossing 0<χd(t0)<1, so Re⁡χd(t0)>∣χd(t0)∣2. The entanglement fidelity of R4 is consequently strictly greater than that of transpose recovery throughout some open time interval containing t0. There are such crossings at arbitrarily large times.

A decoder that corrects the decay-branch phase has fidelity at least as large as R4 at every positive-decay time; the comparison with transpose recovery therefore does not assert that R4 outperforms phase-corrected recovery. If Δ=0 and γt>0, χd=1 and the two compared fidelities tie. If γt=0, the decay branch has zero weight, no normalized decay coherence is assigned, and both recoveries act as the identity on the code.

Facts & Assumptions

[F1]

The postulated model has a two-dimensional code, an orthogonal two-dimensional decay space, real Δ, rate γ≥0, and the stated recovery R4. For γt>0, the decay probability is p=1−e−γt and the conditional recovered decay branch multiplies logical 01 coherence by the displayed χd. Four-level spontaneous-decay model Four-level syndrome recovery Conditional decoded state and decay coherence

[F2]

Under the Axiom of Choice, the unrotated recovered channel has entanglement fidelity F4=1−p(1−Re⁡χd)/2 when p>0. Four-level fidelity measures for the unrotated decoder The Axiom of Choice

[F3]

For p>0, the model's transpose-recovered channel has coherence multiplier (1−p)+p∣χd∣2, and 0<∣χd∣≤1. At p=0 the transpose recovery acts as the identity after noise on the code. Explicit four-level transpose decoder

[F4]

A qubit coherence channel with multiplier λ has entanglement fidelity (1+Re⁡λ)/2. The phase-corrected flagged decoder has overall multiplier (1−p)+p∣χd∣. Qubit coherence channels and fidelity functionals Transpose recovery for a flagged coherence channel

[F5]

The complex exponential is entire with complex derivative equal to itself, and eix=cos⁡x+isin⁡x and ∣eix∣=1 for real x. The real exponential is positive and tends to zero at negative infinity. The complex exponential is entire and its complex derivative is itself exp(x+iy)=eˣ(cos y+i sin y), |exp(x+iy)|=eˣ, and e^iπ+1=0 The exponential tends to +∞ at +∞ and to 0 at -∞

[F6]
[F7]

The real exponential is strictly increasing on R. In particular, if γ>0 and t≥a, then e−γt≤e−γa. The exponential function is strictly increasing

[F8]

For real x, sin⁡(x+π)=−sin⁡x and cos⁡(x+π)=−cos⁡x; moreover sin⁡(π/2)=1, cos⁡(π/2)=0, sin⁡π=0 and cos⁡π=−1. The shifts at x=0 consequently give sin⁡0=0 and cos⁡0=1. Both sine and cosine have period 2π. Also sin⁡(−x)=−sin⁡x and cos⁡(−x)=cos⁡x. Quarter-turn values and shifts by pi/2 and pi The zero sets of sine and cosine and the least positive common period 2 pi Parity and the Pythagorean identity for sine and cosine

[F9]

Sine is increasing on [−π/2,π/2], and cosine is decreasing on [0,π]. With the endpoint values in [F8], this gives sin⁡θ≥0 and cos⁡θ≥0 for 0≤θ≤π/2. Signs, monotonicity intervals, and ranges of sine and cosine

[F10]

For A⊆R, continuity of f:A→R at s∈A means that for every ε>0 some δ>0 makes ∣f(t)−f(s)∣<ε whenever t∈A and ∣t−s∣<δ. Constants, finite sums, scalar multiples and products of continuous real functions are continuous. Their quotient is continuous on the subset where its denominator is nonzero. Continuity of f : A → ℝ at a point of A and on A: the ε-δ condition, its agreement with lim_x → c f(x) = f(c) at a limit point, and continuity at an isolated point Sums, scalar multiples, products, absolute values, maxima, minima and quotients with nonvanishing denominator of continuous functions are continuous, as are constants, the identity and every polynomial function

[F11]

For a logical-qubit channel E, its entanglement fidelity at I/2 is Fe(E)=⟨Φ∣(id⊗E)(∣Φ⟩⟨Φ∣)∣Φ⟩, where ∣Φ⟩=(∣00⟩+∣11⟩)/2 in the ordered reference and logical bases. Entanglement fidelity on a finite logical space

[A1]

Assume the Axiom of Choice as required by the fidelity-comparison supplier. The Axiom of Choice

Proof

Given: The model, recoveries and parameters in the Statement, together with [A1].

Goal: Establish the strict comparison at positive-phase crossings, its persistence and occurrence at arbitrarily large times, and the stated boundary and phase-corrected comparisons.

1.1givenA1F2F3F4F5F11algebra

Using the entanglement-fidelity convention [F11], for p>0, [F2]–[F4] give F4−Ftr=p(Re⁡χd−∣χd∣2)/2. At a positive-phase crossing put r=χd(t0)>0. By [F3], r≤1. If r=1, the displayed formula for χd gives eiΔt0=1+i(Δ/γ)(1−e−γt0). The left side has modulus one by [F5], while the right side has modulus strictly greater than one because γ>0, t0>0 and Δ≠0. Thus 0<r<1 and F4−Ftr=pr(1−r)/2>0.

1.2givenF5F7F8F9algebra

It remains to show that positive-phase crossings occur arbitrarily late. First suppose Δ>0 and set an=2πn/Δ, bn=(2πn+π/2)/Δ for positive integers n, and q(t)=e−γt. Since an→∞, [F5] gives q(an)→0, so every sufficiently large n satisfies q(an)<min⁡(1,Δ/γ). For t∈[an,bn], set θ=Δt−2πn∈[0,π/2]. By [F8], cos⁡(Δt)=cos⁡θ and sin⁡(Δt)=sin⁡θ. By [F9], both are nonnegative; by [F5], cos⁡2θ+sin⁡2θ=∣eiθ∣2=1. Hence (cos⁡θ+sin⁡θ)2=1+2cos⁡θsin⁡θ≥1, so cos⁡θ+sin⁡θ≥1. It follows that γcos⁡θ+Δsin⁡θ≥min⁡(γ,Δ)(cos⁡θ+sin⁡θ)≥min⁡(γ,Δ). Also q(t)≤q(an) by [F7].

1.3givenF5F10algebra

We supply the continuity inputs explicitly. Fix a complex constant c and real s, and put z∗=cs. Differentiability in [F5] gives η>0 such that ∣ez∗+h−ez∗∣≤M∣h∣ for ∣h∣<η, where M=∣ez∗∣+1: for h≠0 the difference quotient is within 1 of ez∗, and for h=0 the inequality is immediate. Given ε>0, take δ=min⁡{η,ε/M}/(∣c∣+1). If ∣t−s∣<δ, substituting h=c(t−s) gives ∣ect−ecs∣<ε. For w=a+ib, a2,b2≤a2+b2=∣w∣2, so ∣Re⁡w∣,∣Im⁡w∣≤∣w∣. Apply these inequalities to w=ect−ecs. Taking c=iΔ and c=−γ, the real functions C(t)=cos⁡(Δt), S(t)=sin⁡(Δt) and q(t)=e−γt are continuous by the Cartesian formula in [F5] and the definition in [F10]. Restricting their domain to any interval preserves the same estimates.

2.1givenF5F6F8F10step 1.2step 1.3algebra

Write W(t)=(γ−iΔ)(eiΔt−q(t)), so χd(t)=γW(t)/[(γ2+Δ2)p(t)]. The prefactor of W is positive on [an,bn]. By [F5] and [F8], Im⁡W(an)=−Δ(1−q(an))<0 and Im⁡W(bn)=γ+Δq(bn)>0. Throughout this interval, step 1.2 gives Re⁡W(t)=γ(cos⁡θ−q(t))+Δsin⁡θ≥min⁡(γ,Δ)−γq(an)>0. The real function Im⁡W(t)=γS(t)−Δ(C(t)−q(t)) is continuous by step 1.3 and [F10], so [F6] gives an interior zero, at which χd is positive real. The endpoint signs show the phase passes from below to above a multiple of 2π within this right-half-plane interval. Every sufficiently large n gives such a crossing, and an→∞. For Δ<0, [F5] and [F8] give e−ix=eix‾ for real x, so the displayed coherence is the complex conjugate of the one for ∣Δ∣; the same construction applies with the phase direction reversed.

2.2givenF5F7F10step 1.1step 1.3algebra

For γ>0 and t>0, [F7] gives q(t)<1, so p(t)=1−q(t)>0 and D(t)=(γ2+Δ2)p(t)>0. Rationalizing the displayed formula for χd gives its real and imaginary parts as u(t)=γ[γ(C(t)−q(t))+ΔS(t)]/D(t) and v(t)=γ[γS(t)−Δ(C(t)−q(t))]/D(t). Step 1.3 and [F10] show that p,D,u,v are continuous on (0,∞): each numerator and denominator is a finite sum of scalar multiples and products of the continuous real functions C,S,q and constants, and each denominator is nonzero on this domain. Since ∣χd∣2=u2+v2, the fidelity difference is the continuous real function G(t)=p(t)(u(t)−u(t)2−v(t)2)/2, again by [F10]. At a crossing t0, step 1.1 gives G(t0)>0. Apply the definition in [F10] with ε=G(t0)/2, and choose a positive radius smaller than both its δ and t0. On the resulting open interval about t0 one has G(t)>G(t0)/2>0.

3.1givenF1F2F3F4algebra∎

By [F4], the phase-corrected fidelity is 1−p(1−∣χd∣)/2. Since Re⁡χd≤∣χd∣, it is at least F4. If Δ=0 and p>0, direct substitution gives χd=1, so [F2] and [F3] give equal fidelity one. If γt=0, [F1] gives zero decay weight and an identity null branch, while [F3] gives identity action for transpose recovery; no normalized decay state is needed. These establish all assertions.

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