Abstract
In this paper, we show how to realize a quantum interface between optical fields and the polarized nuclear spins in a singly charged quantum dot, which is strongly coupled to a high-finesse optical cavity. Effective direct coupling between cavity and nuclear spins is obtained by adiabatically eliminating the (far detuned) excitonic and electronic states.
The requirements for mapping qubit and continuous variable states of cavity or traveling-wave fields to the collective nuclear spin are investigated: for cavity fields, we consider adiabatic passage processes to transfer the states. It is seen that a significant improvement in cavity lifetimes beyond present-day technology would be required for a quantum interface. We then turn to a scheme that couples the nuclei to the output field of the cavity and does not require a long-lived cavity. We show that the lifetimes reported in the literature and the recently achieved nuclear polarization of ∼90% allow both high-fidelity read-out and write-in of quantum information between the nuclear spins and the output field.
We discuss the performance of the scheme and provide a convenient description of the dipolar dynamics of the nuclei for highly polarized spins, demonstrating that this process does not affect the performance of our protocol.
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