2019
DOI: 10.1103/physrevmaterials.3.113802
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Optimizing the formation of depth-confined nitrogen vacancy center spin ensembles in diamond for quantum sensing

Abstract: Spin ensembles of nitrogen vacancy (NV) centers in diamond are emerging as powerful spin-based sensors for magnetic, electric and thermal field imaging with high spatial and temporal resolution. Here we characterize the formation of depth-confined NV center ensembles, activated by electron irradiation in diamond layers grown by plasma enhanced chemical vapor deposition with nitrogen codoping. To do so, we exploit the high magnetic sensitivity of ensembles of NV centers to probe their spin environment as a func… Show more

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Cited by 33 publications
(37 citation statements)
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“…In summary, electron irradiation is preferred to create NV − ensembles optimized for sensing applications (Uedono et al, 1999;Campbell et al, 2002;Twitchen, Geoghegan, and Perkins, 2010), as this method allows for evenly distributed monovacancies to be created throughout the diamond in a timely manner, with less lattice damage than alternative methods. Theoretical calculations predict that monovacancy creation requires electron energies ≳165 keV (Campbell et al, 2002), roughly consistent with experiments observing vacancy creation down to 145 keV (McLellan et al, 2016;Eichhorn, McLellan, and Jayich, 2019). Older, less reliable experiments find vacancy creation for electron irradiation along the [100] direction at 180 keV but not 170 keV (Koike, Parkin, and Mitchell, 1992).…”
Section: Electron Irradiationsupporting
confidence: 72%
“…In summary, electron irradiation is preferred to create NV − ensembles optimized for sensing applications (Uedono et al, 1999;Campbell et al, 2002;Twitchen, Geoghegan, and Perkins, 2010), as this method allows for evenly distributed monovacancies to be created throughout the diamond in a timely manner, with less lattice damage than alternative methods. Theoretical calculations predict that monovacancy creation requires electron energies ≳165 keV (Campbell et al, 2002), roughly consistent with experiments observing vacancy creation down to 145 keV (McLellan et al, 2016;Eichhorn, McLellan, and Jayich, 2019). Older, less reliable experiments find vacancy creation for electron irradiation along the [100] direction at 180 keV but not 170 keV (Koike, Parkin, and Mitchell, 1992).…”
Section: Electron Irradiationsupporting
confidence: 72%
“…The measured data is fit with a mono-exponential function of the form exp [−A NV bath n bath T], where A NV bath ≈ 292 kHz ppm −1 . [26] The results show that the density of P1 groups I-IV are 4.9 ± 0.15, 10.9 ± 0.25, 11.6 ± 0.19, 5.0 ± 0.15 ppm, respectively. 58, E = 0.66, and F = 0.59) suggesting a Lorentzian distributed spin bath, where the decoherence originates from one spin type.…”
mentioning
confidence: 87%
“…Since the main interest of the study is the optimization of NV density during CVD growth, we compare the NV/P1 ratios in the prepared samples A-F. Estimation of NV center density is a difficult task, and proper estimation methods are still under investigations. [19,26] The technique used to perform the NV density estimation is, similar to the one presented in ref. [19].…”
mentioning
confidence: 99%
“…Shallow NVs have been produced both by direct delta-doping [201] and by low energy ion implantation [186]. Near-surface NVs can also be created by converting incorporated nitrogen through low energy electron irradiation [202].…”
Section: Controlling Nv's Distance From the Surfacementioning
confidence: 99%