微波场无激光金刚石磁力计的研制

Pengju Zhao, Haodong Wang, Fei Kong, Zhecheng Wang, Yuhang Guo, Huiyao Yu, Fazhan Shi, Jiangfeng Du
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引用次数: 0

摘要

金刚石中的氮空位中心是一种独特的磁强计。它的原子尺寸可以将大量的NV中心集成在块体金刚石中,灵敏度缩放为1/nNV $1/\sqrt {n_{\rm NV}}$。然而,这种体积传感器需要高功率激光来偏振并读出NV中心。与高功率激光相关的热损伤和附加噪声的增加阻碍了nNV的生长,从而限制了在皮特斯拉水平上的灵敏度。如图所示,一个基于弛豫测量的微波磁强计,其功率密度由弛豫时间T1决定。通过冷却金刚石传感器延长T1(≈s),所需功率密度进一步降低至0.077Wcm−2 $0.077\nobreakspace {\rm Wcm^{-2}}$,为饱和值的≈10−6 $\approx \ 10^{-6}$。本工作为大尺寸金刚石的利用,将金刚石磁强计的灵敏度提高到飞特斯拉级及以上奠定了基础。
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Toward a Laser-Free Diamond Magnetometer for Microwave Fields
The nitrogen-vacancy (NV) center in diamond is a unique magnetometer. Its atomic size enables integrations of a tremendous amount (nNV) of NV centers in a bulk diamond with a sensitivity scaling as 1 / n NV $1/\sqrt {n_{\rm NV}}$ . However, such a bulk sensor requires a high-power laser to polarize and read out the NV centers. The increasing thermal damage and additional noises associated with high-power lasers hinder the growth of nNV, and thus limit the sensitivity at picotesla level. Here, it shows a relaxometry-based microwave magnetometer that the power density is determined by the relaxation time T1. By cooling the diamond sensor to prolong the T1 (≈s), the required power density further reduces to 0.077 Wcm 2 $0.077\nobreakspace {\rm Wcm^{-2}}$ , 10 6 $\approx \ 10^{-6}$ of the saturation value. This work paves the way for the utilization of large-size diamond to promote the sensitivity of diamond magnetometer to femtotesla level and beyond.
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