Non-fidelity 1 − F = 1 − PQ of the full transfer driven by Gaussian pulses plus weak coupling decay versus their duration and delay τ = Δt (see equation (6))
Figure 5. Non-fidelity 1 − F = 1 − PQ of the full transfer driven by Gaussian pulses plus weak coupling decay versus their duration and delay τ = Δt (see equation (6)). Laser parameters are ΩC/2π = 1 MHz, ΔC/2π = 10 MHz, \Omega _B^0/2\pi =200 MHz and \Omega _R^0/2\pi =20 MHz (filled square, blue dashed line), \Omega _B^0/2\pi =400 MHz and \Omega _R^0/2\pi =40 MHz (empty circle, red solid line), \Omega _B^0/2\pi =800 MHz and \Omega _R^0/2\pi =80 MHz (cross, green dot-dashed line), ΔB/2π = 100 MHz, and ΔR = ΔB − ΔC − αCΩC/2.
A stimulated Raman adiabatic passage (STIRAP)-like scheme is proposed to exploit a three-photon resonance taking place in alkaline-earth-metal ions. This scheme is designed for state transfer between the two fine structure components of the metastable D-state which are two excited states that can serve as optical or THz qubit. The advantage of a coherent three-photon process compared to a two-photon STIRAP lies in the possibility of exact cancellation of the first-order Doppler shift which opens the way for an application to a sample composed of many ions. The transfer efficiency and its dependence with experimental parameters are analysed by numerical simulations. This efficiency is shown to reach a fidelity as high as (1–8 × 10−5) with realistic parameters. The scheme is also extended to the synthesis of a linear combination of three stable or metastable states.