Zheng Hui-jie, Quan Wei, Liu Xiang, Chen Yao, Lu Ji-xi
Guang Pu Xue Yu Guang Pu Fen Xi. 2015 Feb;35(2):507-11.
High sensitivitymagnetic measurementscanbe achieved by utilizing atomic spinmanipulation in the spin-exchange-relaxation-free (SERF) regime, which uses an alkali cell as a sensing element. The atomic number density of the alkali vapor and the pressure of the buffer gasare among the most important parameters of the cell andrequire accurate measurement. A method has been proposed and developedto measure the atomic number density and the pressure based on absorption spectroscopy, by sweeping the absorption line and fittingthe experiment data with a Lorentzian profile to obtainboth parameters. Due to Doppler broadening and pressure broadening, which is mainly dominated by the temperature of the cell and the pressure of buffer gas respectively, this work demonstrates a simulation of the errorbetween the peaks of the Lorentzian profile and the Voigt profile caused by bothfactors. The results indicates that the Doppler broadening contribution is insignificant with an error less than 0.015% at 313-513 K for a 4He density of 2 amg, and an error of 0.1% in the presence of 0.6-5 amg at 393 K. We conclude that the Doppler broadening could be ignored under above conditions, and that the Lorentzianprofile is suitably applied to fit the absorption spectrumobtainingboth parameters simultaneously. In addition we discuss the resolution and the instability due to thelight source, wavelength and the temperature of the cell. We find that the cell temperature, whose uncertainty is two orders of magnitude larger than the instability of the light source and the wavelength, is one of the main factors which contributes to the error.
通过在无自旋交换弛豫(SERF)机制中利用原子自旋操控,可以实现高灵敏度的磁性测量,该机制使用碱金属池作为传感元件。碱金属蒸汽的原子数密度和缓冲气体的压力是该池最重要的参数之一,需要精确测量。已经提出并开发了一种基于吸收光谱法来测量原子数密度和压力的方法,即通过扫描吸收线并将实验数据与洛伦兹分布拟合以获得这两个参数。由于多普勒展宽和压力展宽分别主要由池的温度和缓冲气体的压力主导,这项工作展示了对由这两个因素引起的洛伦兹分布峰与沃伊特分布之间误差的模拟。结果表明,对于4He密度为2 amg,在313 - 513 K时,多普勒展宽贡献微不足道,误差小于0.015%;在393 K时,当存在0.6 - 5 amg时,误差为0.1%。我们得出结论,在上述条件下多普勒展宽可以忽略不计,并且洛伦兹分布适用于拟合吸收光谱以同时获得这两个参数。此外,我们还讨论了由于光源、波长和池的温度导致的分辨率和不稳定性。我们发现,池温度的不确定性比光源和波长的不稳定性大两个数量级,是导致误差的主要因素之一。