\begin{document}${6^2}{{\rm{S}}_{1/2}}\;F = 4$\end{document}\begin{document}${6^2}{{\rm{P}}_{1/2}}\;F' = 3$\end{document} transition) and the indirect pump (pump frequency is resonant to \begin{document}${6^2}{{\rm{S}}_{1/2}}\;F = 3 $\end{document}\begin{document}${6^2}{{\rm{P}}_{1/2}}\;F' = 4$\end{document} transition) are analyzed. The experiment is performed based on a 20-mm cube cesium vapour cell with 20-Torr helium as buffer gas. The linearly polarized probe beam is tuned to resonance to cesium D2 transition \begin{document}${6^2}{{\rm{S}}_{1/2}}\;F = 4$\end{document}\begin{document}$ {6^2}{{\rm{P}}_{3/2}}\;F' = 5$\end{document}, and the intensity of the probe is 0.2 W/m2. The spectra of magnetic resonance are measured by using the lock-in detection with a scanning of the modulation frequency. Then the sensitivity can be obtained by measuring MRL and SNR. The experimental results show that the sensitivity and the pump intensity are related nonlinearly, which is coincident with theoretical result. Higher sensitivity can be obtained under the condition of indirect pump. In addition, the effect of atomic spin relaxation on sensitivity is also analyzed with the indirect pump beam. This work clarifies the dynamics of the Bell-Bloom magnetometer to some extent. The highest sensitivity obtained is \begin{document}$31.7\;{\rm{pT}}/\sqrt {{\rm{Hz}}} $\end{document} in our experiment, which can be optimized by using other kinds of vapour cells and different measuring methods."> - 必威体育下载

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Yang Chen, Zuo Guan-Hua, Tian Zhuang-Zhuang, Zhang Yu-Chi, Zhang Tian-Cai
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  • Abstract views:7732
  • PDF Downloads:86
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  • Received Date:06 January 2019
  • Accepted Date:25 February 2019
  • Available Online:01 May 2019
  • Published Online:05 May 2019

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