Steven Chu's Bell Laboratories team prepared sodium atoms by pulsed-laser evaporation of a pellet. A frequency-swept opposing beam slowed them before six crossed laser beams supplied optical molasses. The vacuum chamber used a shield coated with graphite and cooled with liquid nitrogen as a pump. Fluorescence provided the readout; the initial beams were aligned as closely counterpropagating as possible. [ref]
The manipulation of neutral particles by Steven Chu. Steven Chu, The manipulation of neutral particles, 1998 publication of his Nobel lecture, pp. 687–690, Figs. 3–4 and footnote 5: sodium source, precooling, vacuum apparatus, beam geometry and fluorescence detection
.After equilibration, the team switched off the cooling light for a variable interval, then restored it. Faster atoms escaped during the dark interval; slower atoms were recaptured. The recaptured fraction versus delay constrained the velocity distribution and hence temperature. The inference depended on the initial cloud shape and recapture volume: Steven Chu later acknowledged adjusting a geometry correction towards the expected Doppler cooling limit. Delay was the scanned variable, and the cooling beams themselves supplied the release/recapture control; visible fluorescence alone could not establish temperature. [ref]
The manipulation of neutral particles by Steven Chu. Steven Chu, The manipulation of neutral particles, p. 688, release-and-recapture paragraph: measurement sequence and retrospective account of the geometry correction
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