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Volumn 17, Issue 7, 2007, Pages 983-992

Selective reflection spectroscopy on the UV third-resonance line of Cs: Simultaneous probing of a van der Waals atom-surface interaction sensitive to far IR couplings and interatomic collisions

Author keywords

[No Author keywords available]

Indexed keywords

ATOMIC PHYSICS; INTERFACES (MATERIALS); SAPPHIRE; SPECTROSCOPIC ANALYSIS; VAN DER WAALS FORCES;

EID: 34547163913     PISSN: 1054660X     EISSN: 15556611     Source Type: Journal    
DOI: 10.1134/S1054660X07070134     Document Type: Article
Times cited : (24)

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    • No significant deviation to this hypothesis can be established through our various attempts to fit the SR spectra with parameters allowing a dependence on the hyperfine component e.g, for the pressure effect or the vW interaction
    • No significant deviation to this hypothesis can be established through our various attempts to fit the SR spectra with parameters allowing a dependence on the hyperfine component (e.g., for the pressure effect or the vW interaction).
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    • Note that the frequency referencing operated for each individual hyperfine component is responsible for some uncertainties in the frequency scale, owing to micrononlinearities affecting the frequency scan. The relative distance between the components of the SA reference can, indeed, appear in slight disagreement with the expected hyperfine structure.
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    • Even if an absolute calibration of the SR signal often appears to be delicate (e.g., theΔR/R value may be affected by scattering losses for the nonresonant reflection coefficient R), the information on the relative amplitude is significant when comparing spectra solely differing by atomic density.
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    • Our values were mostly obtained when analyzing data for the 6S 1/2(F, 4) → 8P3/2 component, and the experiments for the 6S1/2(F, 3) → 8P3/2 component corresponds to a later series of experiments. Although the same Aλ value is found (see Fig. 8a, smaller pressure broadening and shifts are obtained, which remain, however, compatible with the SA data note that no systematic SA analysis was performed on the SA spectra for the F, 3 → F, 2, 3, 4} component, We suspect a change has occurred in the positioning of our temperature probes, from which the pressure is evaluated
    • 3/2 component corresponds to a later series of experiments. Although the same Aλ value is found (see Fig. 8a), smaller pressure broadening and shifts are obtained, which remain, however, compatible with the SA data (note that no systematic SA analysis was performed on the SA spectra for the F = 3 → F' = {2, 3, 4} component). We suspect a change has occurred in the positioning of our temperature probes, from which the pressure is evaluated.
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