D.J. Whiting
Direct measurement of excited-state dipole matrix elements using electromagnetically induced transparency in the hyperfine Paschen-Back regime
Whiting, D.J.; Keaveney, J.; Adams, C.S.; Hughes, I.G.
Abstract
Applying large magnetic fields to gain access to the hyperfine Paschen-Back regime can isolate three-level systems in a hot alkali metal vapors, thereby simplifying usually complex atom-light interactions. We use this method to make the first direct measurement of the |⟨5P||er||5D⟩| matrix element in Rb87. An analytic model with only three levels accurately models the experimental electromagnetically induced transparency spectra and extracted Rabi frequencies are used to determine the dipole matrix element. We measure |⟨5P3/2||er||5D5/2⟩|=(2.290±0.002stat±0.04syst)ea0, which is in excellent agreement with the theoretical calculations of Safronova, Williams, and Clark [Phys. Rev. A 69, 022509 (2004)].
Citation
Whiting, D., Keaveney, J., Adams, C., & Hughes, I. (2016). Direct measurement of excited-state dipole matrix elements using electromagnetically induced transparency in the hyperfine Paschen-Back regime. Physical Review A, 93(4), Article 043854. https://doi.org/10.1103/physreva.93.043854
Journal Article Type | Article |
---|---|
Acceptance Date | Apr 10, 2016 |
Online Publication Date | Apr 28, 2016 |
Publication Date | Apr 28, 2016 |
Deposit Date | Aug 22, 2016 |
Publicly Available Date | Aug 22, 2016 |
Journal | Physical Review A |
Print ISSN | 2469-9926 |
Electronic ISSN | 2469-9934 |
Publisher | American Physical Society |
Peer Reviewed | Peer Reviewed |
Volume | 93 |
Issue | 4 |
Article Number | 043854 |
DOI | https://doi.org/10.1103/physreva.93.043854 |
Public URL | https://durham-repository.worktribe.com/output/1398626 |
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Copyright Statement
Reprinted with permission from the American Physical Society: Physical Review A 93, 043854 © 2016 by the American Physical Society. Readers may view, browse, and/or download material for temporary copying purposes only, provided these uses are for noncommercial personal purposes. Except as provided by law, this material may not be further reproduced, distributed, transmitted, modified, adapted, performed, displayed, published, or sold in whole or part, without prior written permission from the American Physical Society.
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