Abstract
The study of collisions between excited atoms requires high-intensity atomic beams to achieve detector signals of sufficient strength. Producing large densities of excited rare gas atoms R*(*) is especially difficult, since with conventional sources metastable atoms R* make up a tiny fraction of ≈10−5 of the total beam flux. In such cases, "brightening" the beam is the only way to achieve a sufficiently large flux.
© 1994 IEEE
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