Microwave spectroscopic study of the hyperfine structure of antiprotonic super(3)He

In this work, we describe the latest results for the measurements of the hyperfine structure of antiprotonic super(3)He. Two out of four measurable super-super-hyperfine (SSHF) transition lines of the (n, L) = (36, 34) state of antiprotonic super(3)He were observed. The measured frequencies of the i...

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Veröffentlicht in:Journal of physics. B, Atomic, molecular, and optical physics Atomic, molecular, and optical physics, 2013-06, Vol.46 (12), p.125003-1-9
Hauptverfasser: 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
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container_end_page 1-9
container_issue 12
container_start_page 125003
container_title Journal of physics. B, Atomic, molecular, and optical physics
container_volume 46
creator 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
description In this work, we describe the latest results for the measurements of the hyperfine structure of antiprotonic super(3)He. Two out of four measurable super-super-hyperfine (SSHF) transition lines of the (n, L) = (36, 34) state of antiprotonic super(3)He 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 super(3)He (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 0.03245 (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 plus or minus 0.62 MHz and an inelastic collision rate of gamma i = 0.51 plus or minus 0.07 MHz.
doi_str_mv 10.1088/0953-4075/46/12/125003
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subjects Collisions
Elastic scattering
Helium atoms
Hyperfine structure
Inelastic collisions
Mathematical analysis
Microwaves
Simulation
title Microwave spectroscopic study of the hyperfine structure of antiprotonic super(3)He
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