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arXiv 2103.16221physics.atom-phphysics.data-an
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$^{129}$晶体电偶极矩测量分析的全局相位拟合方法

A global phase fitting approach for the analysis of $^{129}$Xe electric dipole moment measurements

Tianhao Liu

摘要:

测量粒子或系统的永久电偶极矩(EDM)的大小提供了一个强有力的工具来测试超越标准模型物理。反磁性$^{129}$双原子由于其在均匀磁场中具有高的核极化率和较长的自旋相干时间而成为EDM实验中最有希望的候选原子之一。通过测量极化的$^{129}$ He和$^{3}$ He的自旋进动频率,在Phys.Rev.Lett. 123,143003(2019)。本文提出了一种基于全局相位拟合(GPF)的$^{3}$ He-$^{129}$超导磁强计信号连续相位发展分析方法。从理论上推导了GPF方法的$^{129}$离散EDM的Cramer-Rao下界,并证明了该方法在不引入新的系统不确定性的情况下获得高的统计灵敏度的好处。GPF方法的鲁棒性与蒙特卡罗研究进行了验证。通过优化分析参数和增加少量用前一种方法无法分析的数据,得到了\[ { d_\mathrm{A} (^{129}\mathrm{Xe})=(1.1 \pm 3.6_\mathrm{(stat)} \pm 2.0_\mathrm{(syst)})\times 10 ^{-28} e~\mathrm{cm}}, \]的结果,并利用该结果推导出了$^{129}$在95% C. L.下的电火花永久放电上限。\[ {|d_\text{A}(^{129}\text{Xe})| < 8.3 \times 10^{-28}~e~\mathrm{cm}}. \]与之前的结果相比,该限值小1.7倍。

英文摘要:

Measuring the size of permanent electric dipole moments (EDM) of a particle or system provides a powerful tool to test Beyond-the-Standard-Model physics. The diamagnetic $^{129}$Xe atom is one of the promising candidates for EDM experiments due to its obtainable high nuclear polarization and its long spin-coherence time in a homogeneous magnetic field. By measuring the spin precession frequencies of polarized $^{129}$Xe and $^{3}$He, a new upper limit on the $^{129}$Xe atomic EDM $d_\mathrm{A}(^{129}\mathrm{Xe})$ was reported in Phys. Rev. Lett. 123, 143003 (2019). This writeup proposes a new evaluation method based on global phase fitting (GPF) for analyzing the continuous phase development of the $^{3}$He-$^{129}$Xe comagnetometer signal. The Cramer-Rao Lower Bound on the $^{129}$Xe EDM for the GPF method is theoretically derived and shows the benefit of achieving high statistical sensitivity without bringing new systematic uncertainties. The robustness of the GPF method is verified with Monte-Carlo studies. By optimizing the analysis parameters and adding few more data that could not be analyzed with the former method, a result of \[ { d_\mathrm{A} (^{129}\mathrm{Xe})=(1.1 \pm 3.6_\mathrm{(stat)} \pm 2.0_\mathrm{(syst)})\times 10 ^{-28} e~\mathrm{cm}}, \] is obtained and is used to derive the upper limit of $^{129}$Xe permanent EDM at 95\% C.L. \[ {|d_\text{A}(^{129}\text{Xe})| < 8.3 \times 10^{-28}~e~\mathrm{cm}}. \] This limit is a factor of 1.7 smaller as compared to the previous result.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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