[1] TAKAMOTO M,HONG F L,HIGASHI R,et al.An optical lattice clock[J].Nature,2005,435(7040):321-324.
[2] TAN Zh Q,LONG X W.Influence of cavity length change on measurement of CW cavity ring-down[J].Laser Technology,2007,31(4):438-441(in Chinese).
[3] HU Ch X,ZHENG M,DENG T,et al.Influence of air gap on the lasing wavelength of the fiber grating external cavity semiconductor laser[J].Laser Technology,2008,32(2):177-179(in Chinese).
[4] LIN X.Alternative scheme for generation of atomic Schródinger cat states and entangled coherent states in an optical cavity[J].Communications in Theoretical Physics,2010(5):927-930.
[5] TAN Zh Q,LONG X W.Design of driving circuits of semiconductor lasers for measurement of continuous-wave cavity ring-down technology[J].Laser Technology,2008,32(1):27-29(in Chinese).
[6] ZHOU H Q,XIA G Q,DENG T,et al.Influence of external cavity length variation on the lasing wavelength of the fiber grating external cavity semiconductor laser[J].Laser Technology,2005,29(5):476-477(in Chinese).
[7] YOUNGB C,CRUZ F C,ITANO W M,et al.Visible lasers with subhertz linewidths[J].Physical Review Letters,1999,82(19):3799-3802.
[8] SUN X T,LIU J Q,ZHOU J,et al.Confocal Fabry-Perot interferometer for frequency stabilization of laser[J].Chinese Journal of Lasers,2008,35(7):1005-1008(in Chinese).
[9] MIAO J.Study of vibration sensitivity of optical cavities used for stable and narrow line width laser system[D].Shanghai:East China Normal University,2008:16-28(in Chinese).
[10] YANG T.Researching the stabilization of ultra stable Fabry-Perot cavities[D].Beijing:Beijing Jiaotong University,2007:15-28(in Chinese).
[11] CHEN L S,HALL J L,YE J.Vibration-induced elastic deformation of Fabry-Perot cavities[J].Physical Review,2006,A74(5):053801/1-053801/13.
[12] YANG T,LI W B,ZANG E J,et al.Decreased vibrational susceptibility of Fabry-Perot cavities via designs of geometry and structural support[J].Chinese Physics,2007,16(5):1374-1385.