Ultra-stable optical clock with two cold-atom ensembles
arXiv:1607.06867 · doi:10.1038/nphoton.2016.231
Abstract
Atomic clocks based on optical transitions are the most stable, and therefore precise, timekeepers available. These clocks operate by alternating intervals of atomic interrogation with dead time required for quantum state preparation and readout. This non-continuous interrogation of the atom system results in the Dick effect, an aliasing of frequency noise of the laser interrogating the atomic transition. Despite recent advances in optical clock stability achieved by improving laser coherence, the Dick effect has continually limited optical clock performance. Here we implement a robust solution to overcome this limitation: a zero-dead-time optical clock based on the interleaved interrogation of two cold-atom ensembles. This clock exhibits vanishingly small Dick noise, thereby achieving an unprecedented fractional frequency instability of for an averaging time in seconds. We also consider alternate dual-atom-ensemble schemes to extend laser coherence and reduce the standard quantum limit of clock stability, achieving a spectroscopy line quality factor .
References in corpus (6)
- Systematic evaluation of an atomic clock at 2e-18 total uncertainty
- Quantum State Engineering and Precision Metrology using State-Insensitive Light Traps
- Searching for dilaton dark matter with atomic clocks
- Titania-doped tantala/silica coatings for gravitational-wave detection
- A transportable strontium optical lattice clock
- Stability enhancement by joint phase measurements in a single cold atomic fountain
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