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In-beam measurement of the hydrogen hyperfine splitting and prospects for antihydrogen spectroscopy

机译:氢中超细分裂的束流测量和抗氢光谱学的前景

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摘要

Antihydrogen, the lightest atom consisting purely of antimatter, is an ideal laboratory to study the CPT symmetry by comparison with hydrogen. With respect to absolute precision, transitions within the ground-state hyperfine structure (GS-HFS) are most appealing by virtue of their small energy separation. ASACUSA proposed employing a beam of cold antihydrogen atoms in a Rabi-type experiment, to determine the GS-HFS in a field-free region. Here we present a measurement of the zero-field hydrogen GS-HFS using the spectroscopy apparatus of ASACUSA's antihydrogen experiment. The measured value of νHF=1,420,405,748.4(3.4) (1.6) Hz with a relative precision of 2.7 × 10−9 constitutes the most precise determination of this quantity in a beam and verifies the developed spectroscopy methods for the antihydrogen HFS experiment to the p.p.b. level. Together with the recently presented observation of antihydrogen atoms 2.7 m downstream of the production region, the prerequisites for a measurement with antihydrogen are now available within the ASACUSA collaboration.
机译:抗氢是最纯的由反物质组成的最轻的原子,是与氢比较研究CPT对称性的理想实验室。关于绝对精度,基态超精细结构(GS-HFS)内的跃迁因其较小的能量分离而最为吸引人。 ASACUSA建议在Rabi型实验中使用一束冷的抗氢原子,以确定无电场区域的GS-HFS。在这里,我们使用ASACUSA的反氢实验的光谱仪对零场氢GS-HFS进行测量。相对准确度为2.7×10 −9 的νHF= 1,420,405,748.4(3.4)(1.6)Hz的测量值构成了光束中该量的最精确测定,并验证了针对该光束开发的光谱方法ppb的抗氢HFS实验水平。连同最近提出的在生产区域下游2.7μm处观察到的抗氢原子,现在在ASACUSA合作中可以找到进行抗氢测量的先决条件。

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