Microwave spectroscopic study of the hyperfine structure of antiprotonic 3He

被引:8
作者
Friedreich, S. [1 ]
Barna, D. [2 ,3 ]
Caspers, F. [4 ]
Dax, A. [2 ]
Hayano, R. S. [2 ]
Hori, M. [2 ,5 ]
Horvath, D. [3 ,6 ]
Juhasz, B. [1 ]
Kobayashi, T. [2 ]
Massiczek, O. [1 ]
Soter, A. [5 ]
Todoroki, K. [2 ]
Widmann, E. [1 ]
Zmeskal, J. [1 ]
机构
[1] Austrian Acad Sci, Stefan Meyer Inst Subat Phys, A-1090 Vienna, Austria
[2] Univ Tokyo, Dept Phys, Bunkyo Ku, Tokyo 1130033, Japan
[3] Wigner Res Ctr Phys, Inst Particle & Nucl Phys, H-1121 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
基金
奥地利科学基金会; 俄罗斯基础研究基金会; 日本学术振兴会;
关键词
LASER SPECTROSCOPY; HFS TRANSITIONS; LIQUID-HELIUM; CAVITY; STATES; ATOMS;
D O I
10.1088/0953-4075/46/12/125003
中图分类号
O43 [光学];
学科分类号
070207 ; 0803 ;
摘要
In this work, we describe the latest results for the measurements of the hyperfine structure of antiprotonic He-3. Two out of four measurable super-super-hyperfine (SSHF) transition lines of the (n, L) = (36, 34) state of antiprotonic He-3 were observed. The measured frequencies of the individual transitions are 11.125 48(08) GHz and 11.157 93(13) GHz, with the increased precisions of about 43% and 25%, respectively, compared to our first measurements with antiprotonic He-3 (Friedreich et al 2011 Phys. Lett. B 700 1-6). They are less than 0.5 MHz higher with respect to the most recent theoretical values, still within their estimated errors. Although the experimental uncertainty for the difference of 0.032 45(15) GHz between these frequencies is large as compared to that of theory, its measured value also agrees with theoretical calculations. The rates for collisions between antiprotonic helium and helium atoms have been assessed through comparison with simulations, resulting in an elastic collision rate of gamma(e) = 3.41 +/- 0.62 MHz and an inelastic collision rate of gamma(i) = 0.51 +/- 0.07 MHz.
引用
收藏
页数:9
相关论文
共 30 条
[1]  
[Anonymous], COMMUNICATION
[2]   Hyperfine structure of antiprotonic helium energy levels [J].
Bakalov, D ;
Korobov, VI .
PHYSICAL REVIEW A, 1998, 57 (03) :1662-1667
[3]  
Barlow R, 2003, PHYSTAT 03 P STAT PR
[4]  
DiSciacca J., 2013, PHYS REV LETT
[5]  
Fluegge S, 1959, ENCY PHYS, VXXXVII/ I
[6]   First observation of two hyperfine transitions in antiprotonic 3He [J].
Friedreich, S. ;
Barna, D. ;
Caspers, F. ;
Dax, A. ;
Hayano, R. S. ;
Hori, M. ;
Horvath, D. ;
Juhasz, B. ;
Kobayashi, T. ;
Massiczek, O. ;
Soter, A. ;
Todoroki, K. ;
Widmann, E. ;
Zmeskal, J. .
PHYSICS LETTERS B, 2011, 700 (01) :1-6
[7]  
Friedreich S, 2012, THESIS
[8]   Microwave spectroscopy measurements of the hyperfine structure in antiprotonic 3He [J].
Friedreich, Susanne ;
Daniel Barna ;
Caspers, Fritz ;
Dax, Andreas ;
Hayano, Ryugo ;
Hori, Masaki ;
Dezso Horvath ;
Juhasz, Bertalan ;
Kobayashi, Takumi ;
Massiczek, Oswald ;
Soter, Anna ;
Todoroki, Koichi ;
Widmann, Eberhard ;
Zmeskal, Johann .
HYPERFINE INTERACTIONS, 2012, 212 (1-3) :167-177
[9]   Antiprotonic helium and CPT invariance [J].
Hayano, Ryugo S. ;
Hori, Masaki ;
Horvath, Dezsoe ;
Widmann, Eberhard .
REPORTS ON PROGRESS IN PHYSICS, 2007, 70 (12) :1995-2065
[10]   Determination of the antiproton-to-electron mass ratio by precision laser spectroscopy of (p)over-barHe+ [J].
Hori, M. ;
Dax, A. ;
Eades, J. ;
Gomikawa, K. ;
Hayano, R. S. ;
Ono, N. ;
Pirkl, W. ;
Widmann, E. ;
Torii, H. A. ;
Juhasz, B. ;
Barna, D. ;
Horvath, D. .
PHYSICAL REVIEW LETTERS, 2006, 96 (24)