Alkali D Line Data - Steck
3 Hyperfine Structure 5 because ∆ωsw/2πis the beat frequency of the two waves, and λ/2 is the spatial periodicity of the standing wave. For a standing wave velocity of vr, Eq.
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Alkali D Line Data - Steck
steck.us3 Hyperfine Structure 5 trapping experiments are also given here. The recoil temperature is the temperature corresponding to an ensemble with a one-dimensional rms momentum of one photon recoil ~k
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steck.us4 2 Rubidium 85 Physical and Optical Properties to typical laboratory conditions (100 kPa pressure, 20 C temperature, and 50% relative humidity).The index of refraction is calculated from the 1993 revision [13] of the Edl´en formula [14]:
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steck.usbalance of Doppler cooling and recoil heating [13]. Of course, in Zeeman-degenerate atoms, sub-Doppler cooling mechanisms permit temperatures substantially below this limit [14]. 3 Hyperfine Structure 3.1 Energy Level Splittings The 5 2S 1/2 −→ 5 2P 3/2 and 5 2S 1/2 −→ 5 P 1/2 transitions are the components of a fine-structure doublet ...
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steck.us23 January 1998 (revision 1.6, 14 October 2003) 1 Introduction In this reference we present many of the physical and optical properties of cesium that are relevant to various quantum optics experiments. In particular, we giveparameters that are useful in treating the mechanical effects of lighton cesium atoms.
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