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A Method for Measuring the $6S_{1/2} \leftrightarrow 5D_{3/2}$ Magnetic Dipole Transition Moment in {Ba}$^{+}$

机译:一种测量$ 6s_ {1/2} \ leftrightarrow 5D_ {3/2} $ magnetic的方法   {Ba} $ ^ {+} $中的偶极跃迁矩

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摘要

We propose a method for measuring the magnetic dipole (M1) transition momentof the $6S_{1/2} \big(\mathrm{m}=-1/2\big)\leftrightarrow5D_{3/2}\big(\mathrm{m}=-1/2\big)$ transition in single trapped Ba$^{+}$ byexploiting different symmetries in the electric quadrupole (E2) and M1couplings between the states. The technique is adapted from a previouslyproposed method for measuring atomic parity nonconservation in a single trappedion [Norval Fortson, Phys. Rev. Lett. \textbf{70}, 17 (1993)]. Knowledge of M1is crucial for any parity nonconservation measurement in Ba$^{+}$, as lasercoupling through M1 can mimic the parity-violating signal. The magnetic momentfor the transition has been calculated by atomic theory and found to bedominated by electron-electron correlation effects [B.K. Sahoo et. al., Phys.Rev. A \textbf{74}, 6 (2006)]. To date the value has not been verifiedexperimentally. This proposed measurement is therefore an essential step towarda parity nonconservation experiment in the ion that will also test currentmany-body theory. The technique can be adapted for similar paritynonconservation experiments using other atomic ions, where the magnetic dipolemoment could present similar complications.
机译:我们提出了一种测量$ 6S_ {1/2} \ big(\ mathrm {m} =-1/2 \ big)\ leftrightarrow5D_ {3/2} \ big(\ mathrm)的磁偶极(M1)跃迁矩的方法通过利用状态之间的电四极杆(E2)和M1耦合中的不同对称性,在单个陷阱Ba $ ^ {+} $中转变{m} =-1/2 \ big)$。该技术改编自先前提出的用于测量单个陷阱中原子奇偶性不守恒的方法[Norval Fortson,Phys。牧师\ textbf {70},17(1993)]。 M1的知识对于Ba $ ^ {+} $中的任何奇偶校验非保守性测量至关重要,因为通过M1进行的激光耦合可以模仿违反奇偶校验的信号。过渡过程的磁矩已通过原子理论计算得出,并发现受电子-电子相关效应的支配[B.K. Sahoo等等,Phys.Rev。 \ textbf {74},6(2006)]。迄今为止,该值尚未经过实验验证。因此,该拟议的测量方法是朝着离子中的奇偶性非保守性实验迈出的重要一步,该实验还将测试多体理论。该技术可适用于使用其他原子离子的相似奇偶性非保守实验,在该实验中,磁偶极矩可能会表现出相似的复杂性。

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