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Our architecture is similar to that of, so we may use the same methods proposed there to initialize the nuclear spins in the spin-up state. Alternatively, we may read out the electron-spin state (e.g. as described in) or wait until the electron spins relax to the spin-down ground state then apply MW and rf pulse to initialize the electron spins in the spin-up state and then to swap the nuclear- and electron-spin states. According to our simulations, the error in the initial nuclear-spin-up polarization should be kept smaller than 10-4 (or 10-3) in order to maintain FTQC.
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Our architecture is similar to that of, so we may use the same methods proposed there to initialize the nuclear spins in the spin-up state. Alternatively, we may read out the electron-spin state (e.g. as described in) or wait until the electron spins relax to the spin-down ground state then apply MW and rf pulse to initialize the electron spins in the spin-up state and then to swap the nuclear- and electron-spin states. According to our simulations, the error in the initial nuclear-spin-up polarization should be kept smaller than 10-4 (or 10-3) in order to maintain FTQC.
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