Microwave spectroscopy measurements of the hyperfine structure in antiprotonic 3He

被引:2
|
作者
Friedreich, Susanne [1 ]
Daniel Barna [2 ,3 ]
Caspers, Fritz [4 ]
Dax, Andreas [2 ]
Hayano, Ryugo [2 ]
Hori, Masaki [2 ,5 ]
Dezso Horvath [3 ,6 ]
Juhasz, Bertalan [1 ]
Kobayashi, Takumi [2 ]
Massiczek, Oswald [1 ]
Soter, Anna [5 ]
Todoroki, Koichi [2 ]
Widmann, Eberhard [1 ]
Zmeskal, Johann [1 ]
机构
[1] Austrian Acad Sci, Stefan Meyer Inst Subatom Phys, A-1090 Vienna, Austria
[2] Univ Tokyo, Dept Phys, Tokyo 1130033, Japan
[3] KFKI Res Inst Particle & Nucl Phys, H-1525 Budapest, Hungary
[4] CERN, CH-1211 Geneva, Switzerland
[5] Max Planck Inst Quantum Opt, D-85748 Garching, Germany
[6] Hungarian Acad Sci, Inst Nucl Res, H-4001 Debrecen, Hungary
来源
HYPERFINE INTERACTIONS | 2012年 / 212卷 / 1-3期
关键词
Antiproton; Antiprotonic helium; Hyperfine structure; Spectroscopy; Laser; Microwave; Three-body quantum electrodynamics; LIQUID-HELIUM; TRANSITIONS; CAVITY; ATOMS; HFS;
D O I
10.1007/s10751-012-0639-y
中图分类号
O64 [物理化学(理论化学)、化学物理学]; O56 [分子物理学、原子物理学];
学科分类号
070203 ; 070304 ; 081704 ; 1406 ;
摘要
We shall present here the first experimental results for microwave spectroscopy of the hyperfine structure of antiprotonic He-3 and a comparison to numerical simulations of the measurement. Due to the helium nuclear spin, antiprotonic He-3 has a more complex hyperfine structure than antiprotonic He-4 which has already been studied before. Thus a comparison between theoretical calculations and the experimental results will provide a more stringent test of the three-body quantum electrodynamics (QED) theory. The comparison of measured data to simulations allows to investigate the collisional processes between the helium atoms of the target medium and the antiprotonic helium atomcules. The collision rates can not be calculated exactly, but estimated by comparison of numeric simulations with the experimental results. Two out of four super-super-hyperfine (SSHF) transition lines of the (n, L) = (36, 34) state were observed. The measured frequencies of the individual transitions are 11.12559(14) GHz and 11.15839(18) GHz, less than 1 MHz higher than the current theoretical values, but still within their estimated errors. The frequency difference between the two lines also agrees with theoretical calculations.
引用
收藏
页码:167 / 177
页数:11
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