In physics, the strong confinement limit, or "festina lente" limit, is a mode of an atom laser in which the frequency of emission of the Bose–Einstein condensate is less than the confinement frequency of the trap.[1]

References

  1. ↑ "Optical Loading of a Bose–Einstein Condensate" (PDF). Archived from the original (PDF) on 2012-02-25.


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