Selective reflection of laser radiation from submicron layers of Rb and Cs atomic vapors: Applications in atomic spectroscopy
- Authors: Klinger E.1,2, Sargsyan A.1, Leroy C.2, Sarkisyan D.1
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Affiliations:
- Institute for Physical Research
- Laboratoire Interdisciplinaire Carnot de Bourgogne, UMR CNRS 6303
- Issue: Vol 125, No 4 (2017)
- Pages: 543-550
- Section: Atoms, Molecules, Optics
- URL: https://journals.rcsi.science/1063-7761/article/view/192605
- DOI: https://doi.org/10.1134/S1063776117090151
- ID: 192605
Cite item
Abstract
We studied selective reflection (SR) of laser radiation from a window of a nanocell with thickness L ~ λ1,2/2 filled with Rb and Cs atoms, where λ1 = 780 nm and λ2 = 852 nm are the wavelengths resonant with the D2 laser lines for Rb and Cs, respectively. It is demonstrated that the negative derivative of the SR signal profile for L > λ/2 changes to the positive one for L < λ/2. It is shown that the real-time formation of the SR signal profile derivative (SRD) with the spectral width 30–40 MHz and located at the atomic transition is, in particular, a convenient frequency marker of D2 transitions in Rb and Cs. The amplitudes of SRD signals are proportional to the atomic transition probabilities. A comparison with the known saturated absorption (SA) method demonstrated a number of advantages, such as the absence of cross-over resonances in the SRD spectrum, the simplicity of realization, a low required power, etc. An SRD frequency marker also operates in the presence of the Ne buffer gas at a pressure of 6 Torr, which allowed us to determine the Ne–Rb collisional broadening, whereas the SA method is already inapplicable at buffer gas pressures above 0.1 Torr. The realization simplicity makes the SRD method a convenient tool for atomic spectroscopy. Our theoretical model well describes the SRD signal.
About the authors
E. Klinger
Institute for Physical Research; Laboratoire Interdisciplinaire Carnot de Bourgogne, UMR CNRS 6303
Email: david@ipr.sci.arn
Armenia, Ashtarak, 0203; Dijon
A. Sargsyan
Institute for Physical Research
Email: david@ipr.sci.arn
Armenia, Ashtarak, 0203
C. Leroy
Laboratoire Interdisciplinaire Carnot de Bourgogne, UMR CNRS 6303
Email: david@ipr.sci.arn
France, Dijon
D. Sarkisyan
Institute for Physical Research
Author for correspondence.
Email: david@ipr.sci.arn
Armenia, Ashtarak, 0203
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