[1] [1] T. Y. Fan, R. L. Byer. Diode laser pumped solid-state lasers. IEEE J. Quant. Electron., 1988, QE-24(6): 895～912

[2] [2] T. Baer. Large amplitude fluctuations due to longitudinal mode coupling in diode-pumped intrcavity-doubled Nd:YAG lasers. J. Opt. Soc. Am. (B), 1986, 3(9): 1175～1180

[3] [3] A. Askin, G. D. Boyed, J. M. Dziedzic. Resonant optical second harmonic generation and mixing. IEEE J. Quant. Electron., 1966, QE-2(6): 109～123

[4] [4] W. J. Kozlovsky, C. D. Nabors, R. L. Byer. Efficient second harmonic generation of a diode-laser-pumped CW Nd:YAG laser using monolithic MgO:LiNbO3 external resonat cavities. IEEE J. Quant. Electron., 1988, QE-24(6): 913～916

[5] [5] D. C. Gerstenberger, G. E. Tye, R. W. Wallance. Efficient second-harmonic conversion of CW single-frequency Nd:YAG laser light by frequency locking to a monolithic ring frequency doubler. Opt. Lett., 1991, 16(13): 992～994

[6] [6] R. Paschotta, P. Kurz, R. Henking et al.. 82% efficient continous-wave frequency doubling of 1.06 μm with a monolithic MgO:LiNbO3 resonator. Opt. Lett., 1994, 19(17): 1325～1327

[7] [7] J. Feinberg. Photorefractive nonlinear optics. Phys. Today, 1988, 41(10): 46～47

[9] [9] Lin-AnWu, J. Kimble. Interference effects in SHG with a optical cavity. J. Opt. Soc. Am. (B), 1985, 2(5): 697～708

[10] [10] G. D. Boyd, D. A. Klienman. Parametric interaction of focused Guassian beams. J. Appl. Phys., 1968, 39(8): 3597～3639

[11] [11] K. C. Peng, Ling-An Wu, H. J. Kimble. Frequency-stabilized Nd:YAG laser with high output power. Appl. Opt., 1985, 24(7): 938～940