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Spectroscopy of the hyperfine structure of antiprotonic ~4He and ~3He

机译:反质子〜4He和〜3He超细结构的光谱学

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摘要

The spin magnetic moment μ_s~p of the antiproton can be determined by comparing the measured transition frequencies in p~4He~+ with three-body QED calculations. A comparison between the proton and antiproton can then be used as a test of CPT invariance. The highest measurement precision of the difference between the proton and the antiproton spin magnetic moments to date is 0.3%. A new experimental value of the spin magnetic moment of the antiproton was obtained as μ_s~p = -2.7862(83)μN, slightly better than the previously best measurement. This agrees with μ_s~p within 0.24%. In 2009, a new measurement with antiprotonic 3He has been started. A comparison between the theoretical calculations and experimental results would lead to a stronger test of the theory and address systematic errors therein. A measurement of this state will be the first HF measurement on p~3He~+. We report here on the new experimental setup and the first tests.
机译:反质子的自旋磁矩μ_s〜p可以通过将p〜4He〜+中测得的跃迁频率与三体QED计算结果进行比较来确定。然后可以将质子和反质子之间的比较用作CPT不变性的检验。迄今为止,质子和反质子自旋磁矩之差的最高测量精度为0.3%。获得了反质子自旋磁矩的新实验值μ_s〜p = -2.7862(83)μN,比以前的最佳测量值稍好。这与0.24%之内的μ_s〜p一致。 2009年,已经开始使用反质子3He进行新的测量。理论计算和实验结果之间的比较将导致对理论的更强有力的检验并解决其中的系统误差。此状态的测量将是p〜3He〜+上的第一个HF测量。我们在这里报告新的实验设置和首次测试。

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