Abstract
A relatively simple method is described for stabilising a dye laser at a frequency ν = ν0 + νc in the vicinity of an atomic resonance frequency ν0. The Doppler effect is exploited by looking for atomic fluorescence when a laser beam is crossed with an atomic beam at certain angles αi. Absolute preselection of νc (the deviation from resonance) up to ~120 MHz is possible by the choice of αi, and a laser stabilisation to better than 1 MHz is obtained. We apply this stabilisation to collision experiments with velocity-selected excited Na atoms.
Original language | English |
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Pages (from-to) | 305-308 |
Number of pages | 4 |
Journal | Journal of physics e-Scientific instruments |
Volume | 20 |
Issue number | 3 |
DOIs | |
Publication status | Published - Mar-1987 |
Externally published | Yes |