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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.

Direct measurement of excited-state dipole matrix elements using electromagnetically induced transparency in the hyperfine Paschen-Back regime Thumbnail


Authors

D.J. Whiting

J. Keaveney

C.S. Adams



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

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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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