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Bulletin of the American Physical Society

Observation of the $^{1}$S$_{0}$ -- $^3$P$_0$ clock transition at 578 nm in atomic Yb

Tao Hong, Claire E. Cramer, Eryn C. Cook, Warren Nagourney, Norval Fortson

Published May 20, 2005• 0 citations
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An optical atomic clock with 171 Yb atoms is devised and tested. By using a two-stage Doppler cooling technique, the 171 Yb atoms are cooled down to a temperature of 6±3 μK, which is close to the Doppler limit. Then, the cold 171 Yb atoms are loaded into a one-dimensional optical lattice with a wavelength of 759 nm in the Lamb—Dicke regime. Furthermore, these cold 171 Yb atoms are excited from the ground-state 1 S 0 to the excited-state 3 P 0 by a clock laser with a wavelength of 578 nm. Finally, the 1 S 0 – 3 P 0 clock-transition spectrum of these 171 Yb atoms is obtained by measuring the dependence of the population of the ground-state 1 S 0 upon the clock-laser detuning.

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Observation of the 1^{1}1S0_{0}0​ -- 3^33P0_00​ clock transition at 578 nm in atomic Yb
Three-Photon EITA for Observing the 1^{1}1S0→ 3_{0} \rightarrow\,^{3}0​→3P0_{0}0​ Clock Transition in Atomic Yb
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An optical atomic clock with 171 Yb atoms is devised and tested. By using a two-stage Doppler cooling technique, the 171 Yb atoms are cooled down to a temperature of 6±3 μK, which is close to the Doppler limit. Then, the cold 171 Yb atoms are loaded into a one-dimensional optical lattice with a wavelength of 759 nm in the Lamb—Dicke regime. Furthermore, these cold 171 Yb atoms are excited from the ground-state 1 S 0 to the excited-state 3 P 0 by a clock laser with a wavelength of 578 nm. Finally, the 1 S 0 – 3 P 0 clock-transition spectrum of these 171 Yb atoms is obtained by measuring the dependence of the population of the ground-state 1 S 0 upon the clock-laser detuning.