Interconnecting well-functioning, scalable stationary qubits and photonic qubits could substantially advance quantum communication applications and serve to link future quantum processors. Here, we present two protocols for transferring the state of a photonic qubit to a single-spin and to a two-spin qubit hosted in gate-defined quantum dots (GDQD). Both protocols are based on using a localized exciton as intermediary between the photonic and the spin qubit. We use effective Hamiltonian models to describe the hybrid systems formed by the the exciton and the GDQDs and apply simple but realistic noise models to analyze the viability of the proposed protocols. Using realistic parameters, we find that the protocols can be completed with a success probability ranging between 85-97 %.
I. INTODUCTIONSemiconductor quantum-dot devices have demonstrated considerable potential for quantum information applications. A prominent example are gate-defined quantum dots (GDQD), i.e. quantum dots realized in semiconductor heterostructures in which individual electrons are confined by an electrostatic trapping potential. Spin qubits based on GDQD in GaAs/Al x Ga x−1 As heterostructures have demonstrated all key requirements for quantum information processing, such as qubit initialization, readout, 1,2 coherent control 3,4 with high fidelity 5,6 and two-qubit gates. 7,8 Moreover, thanks to their similarity to the transistors used in modern computer chips, these top-down fabricated quantum dots have good prospects for realizing large scale quantum processing nodes. However, unlike self-assembled quantum dots, where excellent optical control and information transfer has been demonstrated, [9][10][11] GDQDs pose a number of challenges when it comes to couple them coherently with light. The problems come from the lack of exciton confinement: while the electron states are confined, the hole states are not. Since in the creation of an exciton the spin of the photo-excited electron is always entangled with the one of the hole, discarding the hole-spin inevitably leads to decoherence of the electron spin. This limits considerably the possibility of optically controlling and manipulating spins in GDQDs, and it hinders their applicability in quantum communications.Despite these difficulties, first steps towards the goal of coherently coupling photons and electron spins in GDQDs have already been made, by trapping and detecting photo-generated carriers in GDQDs, 12 and by proving transfer of angular momentum between photons and electrons. 13 Much of this effort is motivated by the fact that robust spin-photon entanglement is a key requirement for quantum repeaters for long-distance quantum communications, 14 as well as for distributed quantum computing, where different computing nodes based on GDQD are connected by optical channels. 15 One strategy to avoid entanglement between the spins of the electron and the hole is to use g-factor engineering to obtain a much smaller g-factor for the electrons than for holes. [16][17][18] Here we propose a ...