Issue |
EPJ Web of Conferences
Volume 66, 2014
INPC 2013 – International Nuclear Physics Conference
|
|
---|---|---|
Article Number | 05009 | |
Number of page(s) | 4 | |
Section | Fundamental Symmetries and Interactions in Nuclei | |
DOI | https://doi.org/10.1051/epjconf/20146605009 | |
Published online | 20 March 2014 |
https://doi.org/10.1051/epjconf/20146605009
Search for a permanent EDM using laser cooled radioactive atom
1 Cyclotron and Radioisotope Center, Tohoku University, Miyagi 980-8578, Japan
2 Graduate School of Arts and Sciences, University of Tokyo, Tokyo 153-8902, Japan
3 Department of Physics, Tokyo Metropolitan University, Tokyo 192-0397, Japan
4 Department of Applied Physics, Tokyo University of Agriculture and Technology, Tokyo 184-8588, Japan
5 Research Center for Nuclear Physics, Osaka University, Osaka 567-0047, Japan
6 Advanced Science Research Center, Japan Atomic Energy Agency, Ibaraki 319-1184, Japan
7 Department of Physics, Kyoto University, Kyoto 606-8502, Japan
8 Department of Physics, Tohoku University, Miyagi 980-8578, Japan
9 Department of Physics, Kyushu University, Fukuoka 812-8581, Japan
a e-mail: kawamura@cyric.tohoku.ac.jp
b Present address: Progress Technologies Inc.
c Present address: Indian Institute of Technology Roorkee
d Present address: Tokyo Institute of Technology
Published online: 20 March 2014
The search for the electric-dipole moment (EDM) of laser-cooled francium (Fr) atoms could lead to a measurement for the electron EDM. It is predicted that the electron EDM would be enhanced by approximately three orders of magnitude in heavy atoms such as Fr. Laser-cooling and trapping techniques are expected to suppress statistical and systematic errors in precision measurements. The magneto-optical trap was achieved using stable rubidium in a developing factory of laser-cooled radioactive atoms. In light of the results from the rubidium experiments, we found that an upgrade of each apparatus is preferred for Fr trapping.
© Owned by the authors, published by EDP Sciences, 2014
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