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Journal of Atomic and Molecular Physics

Peculiarities of absorption from slow atoms confined between two dielectric walls

Yuanyuan Li

Published Jan 1, 2006• 0 citations
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Abstract

The absorption spectroscopy of atomic vapor film between two dielectric walls with Fabret-Perot effects eliminated(the second surface is ideally antireflection coated) is theoretically studied.It is found that the line-shapes of absorption exhibit a Dicke-narrowing structure in several cases are strongly modified by the incident angle of the field and the ratio of L/λ,where L is the thickness of the film and λ the incident wavelength.As an example,we also discussed the magnitude and the linewidth of absorption versus the incident angle for L/λ=1/2.

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The absorption spectroscopy of atomic vapor film between two dielectric walls with Fabret-Perot effects eliminated(the second surface is ideally antireflection coated) is theoretically studied.It is found that the line-shapes of absorption exhibit a Dicke-narrowing structure in several cases are strongly modified by the incident angle of the field and the ratio of L/λ,where L is the thickness of the film and λ the incident wavelength.As an example,we also discussed the magnitude and the linewidth of absorption versus the incident angle for L/λ=1/2.
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Transmission sub-Doppler spectroscopy with confined atomic vapor film between two dielectric walls is theoretically studied. Because of atoms flying from wall to wall, where they get de-excited, the atom-field interaction time is anisotropic so that the contribution of slow atoms is enhanced, a sub-Doppler transmission spectroscopy (Dicke narrowing effect) can be obtained when the thickness of the film is much small or comparable with the wavelength even at small angle oblique incidence. It is feasible to get a sub-Doppler structure in a new region (L < ?/4) in experiments.
This paper investigates the absorptive reduction and the width narrowing of electromagnetically induced transparency (EIT) in a thin vapour film of λ-type atoms confined between two dielectric walls whose thickness is comparable with the wavelength of the probe field. The absorptive lines of the weak probe field exhibit strong reductions and very narrow EIT dips, which mainly results from the velocity slow-down effects and transient behaviour of atoms in a confined system. It is also shown that the lines are modified by the strength of the coupling field and the ratio of L/λ, with L the film thickness and λ the wavelength of the probe field. A simple robust recipe for EIT in a thin medium is achievable in experiment.
One-photon Dick-narrowing absorption spectroscopy from a thin atomic vapor film can be extended to the two-photon case, in which the sub-Doppler absorption structures are obtained in a cascade three-level system. The periodic line shapes of two photon spectroscopy are similar to one-photon case. It is found that Dicke-narrowing is apparent when L/λ=(2n+1)/2 (n an integer, L the film thickness, and λ the wavelength of the probe field)in the case of one-photon process, and this feature is maintained in the case of two-photon process but not in the one-photon process when L/λ=2n/2. Due to the contribution of atom-wall collision in the cell and the pump-probe scheme, a very narrow structure can be obtained when the pump and the probe fields are in counter-propagation regime.
The coefficient of selective reflection at oblique incidence from two-level atoms confined between two dielectric walls is calculated in this paper. It is found to be related to the transient behaviour of atoms after colliding with the wall and the distribution of the field inside the vapour corresponds to L /λ, with L the thickness of the film and λ the incident wavelength. We find that the sub-Doppler structure is manifest both for normal incidence and small angle oblique incidence. It is feasible to detect the real part of selective reflection in several cases that have not been achieved before.
The features of resonance fluorescence and absorption of resonance laser radiation in atomic vapors in a superthin cell with thickness L of the order of a wavelength lambda are investigated theoretically. Taking into account the Fabry-Perot interference effect, it is found that the dependence of the fluorescence and absorption spectra on the ratio L/lambda is substantially different. Coherent spectral narrowing - the Dicke effect - when L=(2n+1)lambda/2 and broadening of the spectral line when L = n lambda (n is a whole number) are observed in the absorption spectra. This effect is absent in the spector of resonance fluorescence in extended media. It is also shown that the processes of saturation and optical pumping significantly alter the spectral line shape as the laser intensity increases; in particular, additional sub-Doppler dips appear at the frequency of the atomic transitions. Calculated curves are given for the D2 lines of ^85Rb atoms. © 2004 Optical Society of America