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 |
|---|---|
| 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 |
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