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Bound electron g-factor measurement by double-resonance spectroscopy on a fine-structure transition

机译:通过双共振光谱法对精细结构跃迁进行束缚电子g因子测量

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Abstract: Precise determination of bound-electron g-factors in highly charged ions provides stringent tests for state of thenart theoretical calculations. The scope reaches from relativistic electron-correlation effects on the one hand to bound-statenQED terms on the other. Besides, the investigation can contribute to the determination of the fine-structure constant a.Inna first approach with boron-like ions of spinless nuclei (e.g.,n40Arn13+ and 40Ca15+), we will excite the 22P1/2 –22P3/2 fine-nstructure transition with laser radiation and probe microwave transitions between Zeeman sublevels. From this laser-micro-nwave double-resonance technique the g-factor can be determined on a ppb level of accuracy. We have prepared a cryo-ngenic trap assembly with a creation trap and a spectroscopy trap—a half-open compensated cylindrical Penning trap.nArgon gas will be injected through a remotely controlled valve, working at cryogenic temperature and in the field of ansuperconducting magnet. Ions are produced by electron impact ionization and transferred to the spectroscopy trap. In thenfuture, the trap will be connected to the HITRAP facility at GSI, and the method will be applied to hyperfine-structurentransitions of hydrogen-like heavy ions to measure electronic and nuclear magnetic moments. We present important techni-nques employed in the experiment.
机译:摘要:高电荷离子中束缚电子g因子的精确测定为现有理论计算的状态提供了严格的检验。范围从一方面相对论的电子相关效应到另一方面的约束状态QED项。此外,该研究有助于确定精细结构常数。用无旋核的硼状离子(例如,n40Arn13 +和40Ca15 +)的Inna第一方法,我们将激发22P1 / 2 –22P3 / 2精细结构激光辐射的跃迁和塞曼子级之间的探针微波跃迁。通过这种激光-微波双共振技术,可以确定ppb精度的g因子。我们准备了一个具有生成阱和光谱阱的低温-自然阱组件-半开补偿圆柱形Penning阱。将通过远程控制阀注入氩气,该气体在低温和超导磁体领域中工作。离子是通过电子碰撞电离产生的,并转移到光谱陷阱中。将来,陷阱将与GSI的HITRAP设施连接,该方法将应用于类氢重离子的超精细结构跃迁,以测量电子和核磁矩。我们介绍了实验中采用的重要技术。

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    《Canadian Journal of Physics》 |2011年第1期|p.79-84|共6页
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    D. von Lindenfels, N.P.M. Brantjes, and W. Quint. GSIHelmholtzzentrum fu ¨r Schwerionenforschung, Planckstr. 1, D64291 Darmstadt, Germany.G. Birkl. Institut fu ¨r Angewandte Physik, TU Darmstadt,Schlossgartenstrasse 7, D-64289 Darmstadt, Germany.V.M. Shabaev. Department of Physics, St. Petersburg StateUniversity, Oulianovskaya 1, Petrodvorets, St. Petersburg198504, Russia.M. Vogel. Physics Department, Imperial College London,London, SW7 2BW, UK.;

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