的激光光谱学
Randolf Pohl1, François Nez2, Luis M P Fernandes3
1Max-Planck-Institut für Quantenoptik, 85748 Garching, Germany. pohl@uni-mainz.de.
概括
研究人员使用子精确测量了子半径,发现值明显小于以前所接受的值. 这种结果加剧了正在进行的质子半径难题.
科学领域:
- 核物理
- 原子物理
背景情况:
- 最简单的原子核 (一个质子,一个中子) 提供了核力量的关键基准.
- 像电荷半径和极化性这样的Deuteron特性是理解核结构的关键.
- 子 (μd) 是由子和子组成的奇异原子,为这些特性提供了新的探测器.
研究的目的:
- 使用子光谱学精确测量子的平均平方电荷半径 (r(d)).
- 将实验确定的r(d) 与来自CODATA和电子光谱的现有值进行比较.
- 调查潜在较小的r (d) 对质子半径难题的影响.
主要方法:
- 在中测量三种2S-2P转换 (μd).
- 奇特的μd原子的高精度光谱.
- 对实验数据进行分析,以提取 deuteron 电荷半径.
主要成果:
- 确定子电荷半径为r (d) =2.12562 (fm).
- 这个值比CODATA-2010值准确2.7倍.
- 测量的r(d) 比CODATA-2010的值小7.5σ,比电子光谱的值小3.5σ.
结论:
- 使用子精确测量子半径,提供了一个新的,高度准确的值.
- 显著较小的子半径挑战了当前的理解和现有的实验价值.
- 这一发现与同位素转移数据相结合,加剧了质子半径难题,表明质子半径较小.
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