Abstract

Photonic time bin qubits are well suited to transmission via optical fibres and waveguide circuits. The states take the form $\frac{1}{\sqrt{2}}(\alpha \ket{0} + e^{i\phi}\beta \ket{1})$, with $\ket{0}$ and $\ket{1}$ referring to the early and late time bin respectively. By controlling the phase of a laser driving a spin-flip Raman transition in a single-hole-charged InAs quantum dot we demonstrate complete control over the phase, $\phi$. We show that this photon generation process can be performed deterministically, with only a moderate loss in coherence. Finally, we encode different qubits in different energies of the Raman scattered light, demonstrating wavelength division multiplexing at the single photon level.

Highlights

  • Quantum dots (QDs) have unparalleled brightness as single-photon sources and can be embedded in a variety of semiconductor devices and microcavity structures [1,2]

  • By controlling the phase of a laser driving a spin-flip Raman transition in a single-holecharged InAs quantum dot, we demonstrate complete control over the phase, φ

  • The qualities of the photons generated from quantum dots have lagged behind other sources such as trapped atoms and ions, which enable the creation of photons with high indistinguishabilities and controllable temporal profiles via stimulated Raman transitions [3,4,5]

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Summary

INTRODUCTION

Quantum dots (QDs) have unparalleled brightness as single-photon sources and can be embedded in a variety of semiconductor devices and microcavity structures [1,2]. The qualities of the photons generated from quantum dots have lagged behind other sources such as trapped atoms and ions, which enable the creation of photons with high indistinguishabilities and controllable temporal profiles via stimulated Raman transitions [3,4,5]. We show that modulating the phase difference between the driving laser pulses results in the modulation of the phase difference between the time bins of the generated single-photon state, enabling complete control of a time-bin qubit without the use of an interferometer.

Phase modulation
Coherence and deterministic excitation
WAVELENGTH CONTROL
CONCLUSIONS
Findings
METHODS
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