Inherently low probability of success (DLCZ-like)
Full excitation and path erasure (Barret-Kok)
Single-photon reflection
Atom-photon gates (Duan-Kimble)
| Rate | only classical light | no optical excitation | |
|---|---|---|---|
| DLCZ | \( \eta (1-F) \) | ✅ | ❌ |
| BK | \( \eta^2 \) | ✅ | ❌ |
| reflection | \( \eta^2 \) | ❌ | ✅ |
You also need a color center that does not suffer from spectral diffusion or charge state instabilities.
If you end up with significant optical excitation, you also need a way to turn off the hyperfine coupling to the (nuclear) memory.
Desired:
\[\begin{aligned} A=\frac{|00\rangle+|11\rangle}{\sqrt{2}}\\ \end{aligned}\]The hardware generated:
90% chance for \[\begin{aligned} A=\frac{|00\rangle+|11\rangle}{\sqrt{2}}\\ \end{aligned}\] 10% chance for a bit flip on Bob's qubit \[\begin{aligned} C=\frac{|01\rangle+|10\rangle}{\sqrt{2}}\\ \end{aligned}\]
Faster purificaiton simulators¹
n-to-k purification circuits²
Rigorous theory bounds on purification performance³
QuantumClifford.jl and QuantumSavory.jl