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Frequency-stabilized 1520 nm diode laser to rubidium two photon absorption
Conference paper   Open access

Frequency-stabilized 1520 nm diode laser to rubidium two photon absorption

Hsiang-Chen Chui, Sen-Yen Shaw, Yi-Wei Liu, Jow-Tsong Shy, R. Roussev and M.M. Fejer
Lasers and Electro-Optics
2003

Abstract

Frequency;Diode lasers;Absorption;Power system harmonics; Erbium-doped fiber amplifier;Lithium niobate;Waveguide transitions;Erbium-doped fiber lasers;Laser transitions;Power laserslaser mode locking;laser frequency stability;semiconductor lasers;rubidium;laser transitions;optical harmonic generation;laser cavity resonators;optical fibre amplifiers;erbium;lithium compounds;optical waveguidesRb;laser frequency stability;diode laser;rubidium two photon absorption;second harmonic signal;external-cavity diode laser;erbium-doped fiber amplifier;periodical poled lithium niobate waveguide;laser locking; frequency-doubled laser;1520 nm;95 mW;LiNbO/sub 3/
Frequency standards in various frequency regions, from if to visible, have been built using atomic rubidium as an absorber. The optical radiation of the rubidium two-photon transition (5S-5D) at 778 nm has been recommended as the realization of meter by CIPM [1]. In the 5S-5D transition, because of the difference of the Lande g factors between S and D states, the magnetic field must be carefully shielded to avoid any possible shift of transition lines caused by Zeeman Effect [2], [3]. However, the 5S1/2−7S1/2 transition is free from such Zeeman shifts [4], since both the lower and upper levels have the same Lande g factors, and thereby does not require a magnetic shielding. The 5Sl/2−7Sl/2 transitions are capable of providing a standard with a sub MHz accuracy for frequency doubled 1520 nm light sources. For the first time, the two-photon transition of rubidium 5SI/2→7SI/2 was observed using second harmonic signal by doubling an external-cavity diode laser that is amplified by an erbium-doped fiber amplifier in a periodical poled lithium niobate waveguide. We get the efficient second harmonic signal, ~10 mW, of a 95-mW 1520-nm tunable laser system, and directly lock the laser frequency to the Rb5S1/2→7S1/2 transitions.
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