2016
DOI: 10.1088/1367-2630/18/8/083016
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Hyperfine-enhanced gyromagnetic ratio of a nuclear spin in diamond

Abstract: The nuclear spin gyromagnetic ratio can be enhanced by hyperfine coupling to the electronic spin. Here we show wide tunability of this enhancement on a 15 N nuclear spin intrinsic to a single nitrogenvacancy center in diamond. We perform control of the nuclear spin near the ground state level anticrossing (GSLAC), where the enhancement of the gyromagnetic ratio from the ground state hyperfine coupling is maximized. We demonstrate a two order of magnitude enhancement of the effective nuclear gyromagnetic ratio … Show more

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Cited by 34 publications
(22 citation statements)
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“…The measured Rabi frequency Ω m is related to its onresonance value by Ω m = √ Ω 2 + δ 2 , where δ is the detuning from the nuclear spin resonance frequency. We incorporate this unknown, small detuning in our model and fit the experimental data with the Rabi enhancement formulas (5)(6)(7). From the fit, we obtain an estimate of the transverse hyperfine coupling, A ⊥ = −2.62 ± 0.05 MHz, in good agreement with recently published values and with better precision than previously measured.…”
supporting
confidence: 81%
See 1 more Smart Citation
“…The measured Rabi frequency Ω m is related to its onresonance value by Ω m = √ Ω 2 + δ 2 , where δ is the detuning from the nuclear spin resonance frequency. We incorporate this unknown, small detuning in our model and fit the experimental data with the Rabi enhancement formulas (5)(6)(7). From the fit, we obtain an estimate of the transverse hyperfine coupling, A ⊥ = −2.62 ± 0.05 MHz, in good agreement with recently published values and with better precision than previously measured.…”
supporting
confidence: 81%
“…Here we show how to meet these two requirements by exploiting nominally forbidden transitions in a hybrid electronic-nuclear spin system associated with the Nitrogen-Vacancy center in diamond 3 . Specifically, we use second-order effects due to mixing of the electronic and nuclear spin states 4 in order to identify with high precision their coupling strength and to enhance the nuclear spin nutation rate 5 .…”
mentioning
confidence: 99%
“…22 The m s = ±1 states move away from the zero magnetic field state at ±28.02 MHz mT −1 . 28 An applied microwave field, tuned to be resonant either with the m s = 0 ↔ +1 or m s = 0 ↔ −1 transition, will flip the spin state.…”
Section: Microwave Controlmentioning
confidence: 99%
“…We choose a 13 C that is sufficiently close to the NV spin to allow for a coherent coupling, 16 yet distant enough to avoid significant hyperfine enhancement of the nuclear Rabi frequency. 34 Our pulse sequence, sketched in Fig. 5(a), consists of three steps: (i) polarization of the 13 C nuclear spin, (ii) nuclear Rabi pulse of variable duration t, and (iii) detection of the ⟨Iz⟩ projection via nuclear state tomography.…”
Section: Nuclear Rabi Rotationsmentioning
confidence: 99%