| 摘要(中) |
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。 |
| 摘要(英) |
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. |
| 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)
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[6]Simon Hooker, Colin Webb, "Laser Physics"
[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)
[8] Jun Ye, Steven T. Cundiff, "Femtosecond Optical Frequency Comb: Principle, Operation, and Applications"
[9] David J. Jones, Scott A. Diddams, Jinendra K. Ranka, Andrew Stentz, Robert S. Windeler, John L. Hall, Steven T. Cundiff, "Carrier-Envelope Phase Control of Femtosecond Mode-Locked Lasers and Direct Optical Frequency Synthesis", Science, Vol. 288 (2000)
[10] Chien-Ming Wu , "Optical frequency comb laser system and Cesium 6S-8S two-photon transition spectroscopy" (2013)
[11] Corney, Alan, "Atomic and laser spectroscopy"
[12] C. S. Wood, S. C. Bennett, D. Cho, B. P. Masterson, J. L. Roberts, C. E. Tanner, C. E. Wieman, "Measurement of Parity Nonconservation and an Anapole Moment in Cesium", Science, Vol. 275 (1997) |
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