An ensemble of two-level atoms is used to estimate an unknown angular frequency by…

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

Quantum Information and Technology, Ch Quantum metrology and sensing

Problem

An ensemble of NN two-level atoms is used to estimate an unknown angular frequency ω\omega by Ramsey interferometry, either as NN independent atoms or as a single NN-atom GHZ state (∣0⟩⊗N+∣1⟩⊗N)/2(|0\rangle^{\otimes N}+|1\rangle^{\otimes N})/\sqrt2. Each atom suffers independent dephasing with single-atom coherence time T2T_2, so that after a free-precession time tt a single atom's Ramsey fringe has visibility V(t)=e−t/T2V(t)=e^{-t/T_2}, and the NN-atom GHZ fringe (which oscillates as cos⁡(Nωt)\cos(N\omega t)) has visibility e−Nt/T2e^{-Nt/T_2}. A total measurement time T\mathcal{T} is available, split into repeated shots of free-precession time tt, giving T/t\mathcal{T}/t shots. For a two-outcome fringe of visibility VV read at its optimal working point, the Fisher information about the phase actually read out, Θ\Theta, is F(Θ)=V2F(\Theta)=V^2 per shot, and Fisher information adds over independent shots (and, for independent atoms, over atoms). ((a)) For NN independent atoms, with Θ=ωt\Theta=\omega t for each, show that the total Fisher information about ω\omega accumulated over the whole time T\mathcal{T} is Findep(t)=NTt e−2t/T2F_{\rm indep}(t)=N\mathcal{T}t\,e^{-2t/T_2}, and find the shot length tt that maximises it. ((b)) For the NN-atom GHZ state, with Θ=Nωt\Theta=N\omega t, show that the total Fisher information is FGHZ(t)=N2Tt e−2Nt/T2F_{\rm GHZ}(t)=N^2\mathcal{T}t\,e^{-2Nt/T_2}, and find the shot length that maximises it. ((c)) Evaluate each maximised Fisher information and hence the best achievable Δω\Delta\omega for both schemes, and show that the GHZ state gives no improvement over independent atoms once each scheme uses its own optimal shot length. ((d)) State, without further calculation, the largest factor by which any entangled state of the NN atoms could beat independent atoms under this noise model.

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