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Note that this approximation is justified only in the regime of a friction force linear in velocity, i.e., well below the capture range of the Sisyphus cooling [Eq. (28)]. For very light atoms, where the capture range is rather small, the cooling of hot atoms is much less efficient, and thus the spatial diffusion can be much larger than the value given by Eq. (32)
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Note that this approximation is justified only in the regime of a friction force linear in velocity, i.e., well below the capture range of the Sisyphus cooling [Eq. (28)]. For very light atoms, where the capture range is rather small, the cooling of hot atoms is much less efficient, and thus the spatial diffusion can be much larger than the value given by Eq. (32).
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Although we focused this paper on the case of the (Formula presented) configuration, we also made some calculations for the (Formula presented) case. In that situation a Sisyphus cooling occurs in the transverse plane because of the phase and intensity variations of the speckle field. However, the temperature is generally higher than the one found in the (Formula presented) configuration
-
Although we focused this paper on the case of the (Formula presented) configuration, we also made some calculations for the (Formula presented) case. In that situation a Sisyphus cooling occurs in the transverse plane because of the phase and intensity variations of the speckle field. However, the temperature is generally higher than the one found in the (Formula presented) configuration.
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