2021
DOI: 10.48550/arxiv.2110.10950
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Cavity Quantum Electrodynamics Effects with Nitrogen Vacancy Center Spins in Diamond and Microwave Resonators at Room Temperature

Yuan Zhang,
Qilong Wu,
Shi-Lei Su
et al.

Abstract: Cavity quantum electrodynamics (C-QED) effects, such as Rabi splitting, Rabi oscillations and superradiance, have been demonstrated with nitrogen vacancy center spins in diamond in microwave resonators at cryogenic temperature. In this article we explore the possibility to realize strong collective coupling and the resulting C-QED effects with ensembles of spins at room temperature. Thermal excitation of the individual spins by the hot environment leads to population of collective Dicke states with low symmetr… Show more

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Cited by 1 publication
(4 citation statements)
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“…To proceed, we firstly translate the spin population polarization into the average of the Dicke states numbers J, M to illustrate more intuitively the collective coupling strength. In our previous study [14], we show that these averaged numbers can be calculated as M = J 0 (2p − 1), J(J + 1) = (2p − 1) 2 J 0 (J 0 + 1) + 6p(p − 1)J 0 with shows the dynamics of the normalized intra-resonator photon number for the laser power 0.01, 0.3, 1, 10 W (black solid, blue dashed, red dash-dotted and green solid line), where the curves are vertically shifted for the sake of clarity. Panel (c) shows the steady-state intra-resonator photon number as function of the detuning of the microwave driving field frequency ω d and the microwave resonator frequency ωc for the laser power 0.01, 0.3, 1, 10 W(black solid, blue dashed, red dash-dotted and green solid line).…”
Section: Room Temperature C-qed Effectsmentioning
confidence: 89%
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“…To proceed, we firstly translate the spin population polarization into the average of the Dicke states numbers J, M to illustrate more intuitively the collective coupling strength. In our previous study [14], we show that these averaged numbers can be calculated as M = J 0 (2p − 1), J(J + 1) = (2p − 1) 2 J 0 (J 0 + 1) + 6p(p − 1)J 0 with shows the dynamics of the normalized intra-resonator photon number for the laser power 0.01, 0.3, 1, 10 W (black solid, blue dashed, red dash-dotted and green solid line), where the curves are vertically shifted for the sake of clarity. Panel (c) shows the steady-state intra-resonator photon number as function of the detuning of the microwave driving field frequency ω d and the microwave resonator frequency ωc for the laser power 0.01, 0.3, 1, 10 W(black solid, blue dashed, red dash-dotted and green solid line).…”
Section: Room Temperature C-qed Effectsmentioning
confidence: 89%
“…In this section, we demonstrate that it can be also utilized to realize the collective strong coupling with the cooled microwave mode, and to manifest the cavity-QED effects at room temperature. These effects have been studied previously by us [14] with a model, which treats the NV spins as two-level systems and the optical spin cooling effectively with single spin relaxation rate. Here, with the more advanced model, we are able to estimate the laser power required to observe these C-QED effects, which can guide directly the experimental research in future.…”
Section: Room Temperature C-qed Effectsmentioning
confidence: 99%
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