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  • 學位論文

銫原子 6S-6D 雙光子超精細耦合常數

Cesium 6S-6D two-photon transitions and hyperfine coupling constants

指導教授 : 鄭王曜
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摘要


我們建立了一套 885 nm 穩頻雷射系統,透過電光調製器光纖,將雷射鎖在銫原子6S1/2 F=3到6D3/2 F=5的交叉譜線上,掃描銫原子6S1/2 F=4 到6D3/2 F=2,3,4,5的躍遷;同樣地,我們將雷射鎖在銫原子6S1/2 F=4 到6D3/2 F=3的交叉譜線上,掃描銫原子6S1/2 F=3到6D3/2 F=2,3,4,5的躍遷,藉此便可得到銫原子6D 3/2的超精細結構。此次我們所量得的 6S 1/2 F=3 到6D 3/2 F=2,3,4,5的躍遷間距分別為,81.767(29) MHz、65.315(19) MHz、49.148(23) MHz,其超精細耦合常數 A 與 B 分別為 16.346(2)、0.058(17);S 1/2 F=4 到6D3/2 F=2,3,4,5的躍遷間距分別為, 81.763(17) MHz、65.320(19) MHz、49.149(3) MHz,其超精細耦合常數 A 與 B 分別為 16.331(3)、0.067(16)。 建立 885 nm 穩頻雷射的另一個目的是為了作為光梳雷射的參考頻率,透過我們實驗室的 822 nm 穩頻雷射,與此次我們所建立的885 nm 穩頻雷射,便可回授控制鈦藍寶石雷射的腔長,鎖住脈衝重覆率,以及回授控制AOM,鎖住鈦藍寶石雷射的偏移頻率,便可得到一穩定之光梳雷射。將頻率鎖在銫原子6S-8S躍遷(822 nm)與6S-6D躍遷(885 nm)的光梳頻雷射,其短期頻率穩定度優於以銫原子鐘做為參考的自參考光梳雷射。

並列摘要


We constructed an 885 nm frequency stabilized diode laser system. We locked the 885 nm laser to Cs atom 6S1/2 F=3 to 6D 3/2 F=5 transition and scanned the frequency of carrier of the diode laser to obtain the hyperfine structure of 6D3/2. Similarly, we locked the 885 nm laser frequency to Cs atom 6S 1/2 F=4 to 6D3/2 F=3 transition and scanned the frequency of carrier of the diode laser to obtain hyperfine structure of 6D3/2. In the end, we deduced that the hyperfine coupling constant via the measuring of 6D3/2 hyperfine interval. In this work, for the hyperfine interval of 6S1/2 F=3 to 6D 3/2 F=2 to 5 that we measured were 81.767(29) MHz, 65.315(19) MHz and 49.148(23) MHz. The hyperfine coupling constants A and B that we deduced were 16.346(2) and 0.058(17). Similarly, the hyperfine interval of 6S1/2 F=4 to 6D3/2 F=2 to 5 that we measured were 81.763(17) MHz, 65.320(19) MHz and 49.149(3) MHz. The hyperfine coupling constants A and B that we deduced were 16.331(3) and 0.067(16) Other purposes of this work are to provide a frequency reference for Ti-Sapphire laser. In the past, our lab made a self-reference comb laser by referring to a Cs clock. In this work, we constructed a stabler frequency comb laser by directly referring the mode-locked laser to a cesium atom two-photon transition at 822 nm and 885 nm.

並列關鍵字

cesium hyperfine coupling constants

參考文獻


[1] Tomoaki Ohtsuka, Nobuo Nishimiya, Takako Fukuda and Masao Suzuki, "Doppler-Free Two-Photon Spectroscopy of 6S 1/2 -6D 3/2, 5/2 Transition in Cesium", J. Phys. Soc. Jpn., Vol. 74, No. 9 (2005)
[2] Vladislav Gerginov, Andrei Derevianko, and Carol E.Tanner, "Observation of the Nuclear Magnetic Octupole Moment of 133 Cs", Phys. Rev. Lett, Vol. 91, No. 7 (2003)
[3] A. Kortyna, N. A. Masluk and T. Bragdon, "Measurement of the 6d 2 D J hypefine structure of cesium using resonant two-photon sub-Doppler spectroscopy", Phys. Rev. A, Vol. 74 (2006)
[4] C. Tai, W. Happer, and R. Gupta, "Hyperfine structure and lifetime measurements of the second-excited D states of rubidium and cesium by cascade fluorescence spectroscopy", Phys. Rev. A, Vol. 12, No. 3 (1975)
[7] T.W. Hansch and B. Couillaud, "Laser Frequency Stabilization by Polarization Spectroscopy of a Reflecting Reference Cavity", Opt. Commun, Vol. 35, No. 3 (1980)

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