Abstract
Narrow-linewidth continuous wave lasers are indispensable tools in experiments based on ultra-cold atoms like optical clocks or quantum computers [1]. Cooling and pumping of the atoms is typically done with commercially available external-cavity diode lasers (ECDL) with linewidths on the order of 100 kHz. Driving the so-called clock transition requires lasers with frequency noise (FN) which is orders of magnitude smaller than in those systems.
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