[1] [1] Bosenberg W R, Cheng L K, Tang C L. Ultraviolet optical parametric oscillation in β-BaB2O4. Appl. Phys. Lett., 1989, 54(1):13～15

[2] [2] Ringling J, Kittelmann O, Noack F. Tunable femtosecond pulse in the near vacuum ultraviolet generated by frequency conversion of amplified Ti: sapphire laser pulses. Opt. Lett., 1993, 18(23): 2035～2037

[4] [4] Mori Y, Kuroda I, Nakajima S et al.. New nonlinear optical crystal: Cesium lithium borate. Appl. Phys. Lett., 1995, 67(13): 1818～1820

[6] [6] Yap Y K, Haramura S, Taguchi A et al.. CsLiB6O10 crystal for frequency doubling the Nd∶YAG laser. Opt. Commun., 1998, 145: 101～104

[7] [7] Yasuke M, Kuroda I, Nakajima S et al.. Nonlinear optical properties of Cesium lithium borate. Jpn. J. Appl. Phys., 1995, 34(3A): L296～L298

[8] [8] Petro V, Noack F, Rotermund F. Sum-frequency generation of femtosecond pulses in CsLiB6O10 down to 175 nm. Appl. Opt., 2000, 39(20): 5076～5078

[11] [11] Nobuhiro U, Kiyoshi K. Ultraviolet generation tunable to 0.185 μm in CsLiB6O10. Appl. Opt., 1997, 36(27): 6794～6796

[12] [12] Hiu Hang, Yao Jianquan, Puri A. Second and third harmonic generation in BBO by femtosecond Ti:sapphire laser pulses. Opt. Commun., 1994, 109(1): 139～144

[13] [13] Wang Li, Chen Shaohua. Optical properties of the second harmonic generation for nonlinear CsLiB6O10. Proc. SPIE, 2001, 4453:18～21