A post-selected linear-optical controlled- gate (success probability

PHYSICS · Multi-part · Fermi University Physics · Quantum Information & Technology · Physical realizations and quantum technologies · Physical realizations and quantum technologies

Quantum Information and Technology, Ch Trapped ions, neutral atoms, photons, NMR and spins in solids

Problem

A post-selected linear-optical controlled-ZZ gate (success probability 1/91/9, quoted) is used, followed by local operations, to herald a photonic Bell pair. State tomography gives a measured squared fidelity (the squared-type quantity hardware papers quote, as defined for average and process fidelities) against ∣Φ+⟩|\Phi^+\rangle of F2=0.95F^2 = 0.95. ((a)) Find the root fidelity F=∣⟨Φ+∣ψ⟩∣F = |\langle\Phi^+|\psi\rangle| used for pure-state overlaps. ((b)) Model the heralded state as a Werner-type mixture ρ=w∣Φ+⟩⟨Φ+∣+(1−w)I/4\rho = w|\Phi^+\rangle\langle\Phi^+| + (1-w)I/4, for which F2=w+(1−w)/4F^2 = w + (1-w)/4. Find the weight ww, and use the Werner-state entanglement condition (w>1/3w > 1/3 for entanglement) to state whether the heralded pair is entangled. ((c)) The combined success probability of the gate together with 90%90\% photon-detection efficiency per photon is p=(1/9)×0.92p = (1/9)\times0.9^2. If attempts are made at 10810^8 per second, estimate the mean time to obtain one successful heralded pair, and compare it with a superconducting two-qubit gate (Chapter 17's datasheet figures) that succeeds essentially deterministically in 60 ns60\,\mathrm{ns}.

Browse the problem library