2012
DOI: 10.1364/oe.20.027198
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Deterministic generation of an on-demand Fock state

Abstract: We theoretically study the deterministic generation of photon Fock states on-demand using a protocol based on a Jaynes Cummings quantum random walk which includes damping. We then show how each of the steps of this protocol can be implemented in a low temperature solid-state quantum system with a Nitrogen-Vacancy centre in a nanodiamond coupled to a nearby high-Q optical cavity. By controlling the coupling duration between the NV and the cavity via the application of a time dependent Stark shift, and by increa… Show more

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Cited by 13 publications
(3 citation statements)
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“…In 2010, Togan et al [34] realized the quantum entanglement generation of an optical photon and an NV center. Photon Fock states on-demand can be implemented in a low-temperature solid-state quantum system with an NV center in a nano-diamond coupled to a nearby high-Q optical cavity [35].…”
Section: Introductionmentioning
confidence: 99%
“…In 2010, Togan et al [34] realized the quantum entanglement generation of an optical photon and an NV center. Photon Fock states on-demand can be implemented in a low-temperature solid-state quantum system with an NV center in a nano-diamond coupled to a nearby high-Q optical cavity [35].…”
Section: Introductionmentioning
confidence: 99%
“…It can be an InAs self-assembled QD grown on the silicondioxide/silicon substrates [62][63][64] Initialization of the QD in either ground state has been experimentally demonstrated with a near-unity probability [65][66][67]. The polarization-selective transition, |1/2 ↔ |3/2 or | − 1/2 ↔ | − 3/2 , can also be tuned to have different energies via the optical Stark effect (OSE) [68][69][70][71][72][73]. For simplicity, we assume that the QD is completely populated in the spin up ground state, or only allows the σ + −polarized transition, enabled by the OSE.…”
mentioning
confidence: 99%
“…We prepare the ancillary mode in the Fock state |n = 1 and evolve by Ĥψ , such that e −i Ĥψ π/2 |G |n = 1 = −i f † |G |n = 0 and we have the excited state up to a phase with no entanglement left between the ancilla and the register. Note the Fock state |n = 1 is a non-Gaussian state, however it can be prepared efficiently by a variety of techniques (see [22] and references therein).…”
mentioning
confidence: 99%