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Bulletin of the American Physical Society

Doppler-free two-photon spectroscopy of Cs $6S_{1/2}$-$7D_{3/2,\,5/2}$ transition

Chin‐Chun Tsai, Yi-Hsiu Chang, Yingyu Chen, Yi-Chih Lee, Hsiang‐Chen Chui

Published May 23, 2009• 0 citations
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Doppler-free two-photon spectroscopy of Cs 6S1/26S_{1/2}6S1/2​-7D3/2, 5/27D_{3/2,\,5/2}7D3/2,5/2​ transition
Two-Photon Polarization Spectroscopy of atomic Cs over the 6s2S1/2→6p2P3/2→9d2D5/26s^{2}S_{1/2}\rightarrow6p^{2}P_{3/2}\rightarrow9d^{2}D_{5/2}6s2S1/2​→6p2P3/2​→9d2D5/2​ transition
The two-photon transition of 87{}^{87}87Rb ($5{S}_{1/2}\ensuremath{-}4{D}_{3/2}$, $5{S}_{1/2}\ensuremath{-}4{D}_{5/2}$) in a vapor cell is investigated with direct frequency-comb spectroscopy. When strong chirp is imposed on a frequency comb, it is found that the Doppler-free signal amplitude barely degrades despite a significant reduction in peak intensity. In addition, it is found that the Doppler-broadened signal is strongly dependent on the applied chirp. We present a simple model that explains this counterintuitive behavior based on the elongated spatial extent of chirped pulses. Keeping Doppler-free signals almost constant, Doppler-broadened background signals can be strongly suppressed with chirped-pulse excitations. Consequently, in the case of uniformly distributed target atoms, chirped-pulse direct frequency-comb spectroscopy can be a useful method to improve the signal-to-noise ratio in two-photon direct frequency-comb spectroscopy.