Precision measurement of transverse velocity distribution of a strontium atomic beam
We measure the transverse velocity distribution in a thermal Sr atomic beam precisely by velocity-selective saturated fluorescence spectroscopy. The use of an ultrastable laser system and the narrow intercombination transition line of Sr atoms mean that the resolution of the measured velocity can re...
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doaj-4f3efd54627a4fa8a1cac9d0f6a050392020-11-24T20:59:26ZengAIP Publishing LLCAIP Advances2158-32262014-02-0142027118027118-610.1063/1.4866983020402ADVPrecision measurement of transverse velocity distribution of a strontium atomic beamF. Gao0H. Liu1P. Xu2X. Tian3Y. Wang4J. Ren5Haibin Wu6Hong Chang7CAS Key Laboratory of Time and Frequency Primary Standards, National Time Service Center, Xi'an 710600, ChinaCAS Key Laboratory of Time and Frequency Primary Standards, National Time Service Center, Xi'an 710600, ChinaCAS Key Laboratory of Time and Frequency Primary Standards, National Time Service Center, Xi'an 710600, ChinaCAS Key Laboratory of Time and Frequency Primary Standards, National Time Service Center, Xi'an 710600, ChinaCAS Key Laboratory of Time and Frequency Primary Standards, National Time Service Center, Xi'an 710600, ChinaCAS Key Laboratory of Time and Frequency Primary Standards, National Time Service Center, Xi'an 710600, ChinaState Key Laboratory of Precision Spectroscopy, Department of Physics, East China Normal University, Shanghai 200062, ChinaCAS Key Laboratory of Time and Frequency Primary Standards, National Time Service Center, Xi'an 710600, ChinaWe measure the transverse velocity distribution in a thermal Sr atomic beam precisely by velocity-selective saturated fluorescence spectroscopy. The use of an ultrastable laser system and the narrow intercombination transition line of Sr atoms mean that the resolution of the measured velocity can reach 0.13 m/s, corresponding to 90 μK in energy units. The experimental results are in very good agreement with the results of theoretical calculations. Based on the spectroscopic techniques used here, the absolute frequency of the intercombination transition of 88Sr is measured using an optical-frequency comb generator referenced to the SI second through an H maser, and is given as 434 829 121 318(10) kHz.http://dx.doi.org/10.1063/1.4866983 |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
F. Gao H. Liu P. Xu X. Tian Y. Wang J. Ren Haibin Wu Hong Chang |
spellingShingle |
F. Gao H. Liu P. Xu X. Tian Y. Wang J. Ren Haibin Wu Hong Chang Precision measurement of transverse velocity distribution of a strontium atomic beam AIP Advances |
author_facet |
F. Gao H. Liu P. Xu X. Tian Y. Wang J. Ren Haibin Wu Hong Chang |
author_sort |
F. Gao |
title |
Precision measurement of transverse velocity distribution of a strontium atomic beam |
title_short |
Precision measurement of transverse velocity distribution of a strontium atomic beam |
title_full |
Precision measurement of transverse velocity distribution of a strontium atomic beam |
title_fullStr |
Precision measurement of transverse velocity distribution of a strontium atomic beam |
title_full_unstemmed |
Precision measurement of transverse velocity distribution of a strontium atomic beam |
title_sort |
precision measurement of transverse velocity distribution of a strontium atomic beam |
publisher |
AIP Publishing LLC |
series |
AIP Advances |
issn |
2158-3226 |
publishDate |
2014-02-01 |
description |
We measure the transverse velocity distribution in a thermal Sr atomic beam precisely by velocity-selective saturated fluorescence spectroscopy. The use of an ultrastable laser system and the narrow intercombination transition line of Sr atoms mean that the resolution of the measured velocity can reach 0.13 m/s, corresponding to 90 μK in energy units. The experimental results are in very good agreement with the results of theoretical calculations. Based on the spectroscopic techniques used here, the absolute frequency of the intercombination transition of 88Sr is measured using an optical-frequency comb generator referenced to the SI second through an H maser, and is given as 434 829 121 318(10) kHz. |
url |
http://dx.doi.org/10.1063/1.4866983 |
work_keys_str_mv |
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