[1] V. L. Vinetskii, N. V. Kukhtarev, S. G. Odulv et al.. Transformation of intensities and phases of light beams by a transient "undisplaced" holographic grating. Phys. Rev. (A), 1987, 35(11): 4680～4683

[2] M. B. Klein. Beam coupling in undoped GaAs at 1.06 μm using the photorefractive effect. Opt. Lett., 1984, 9(8): 350～352

[3] K. Jarasiunas, H. J. Gerritsen. Ambipolor diffusion measurements in semiconductors using nonlinear transient gratings. Appl. Phys. Lett., 1978, 33(2): 190～193

[4] H. J. Eichler, P. Günter, D. W. Pohl. Laser-Induced Dyamic Gtratings. Vol.5 of Springer Series in Optical Science, Berlin: Springer-Verlag, 1986

[5] A. Krumins, P. Gunter. Diffraction efficiency and energy transfer during hologram formation in reduced KNbO3. Appl. Phys., 1979, 19(2): 153～163

[6] H. J. Eichler, M. Glotz, A. Kummrow et al.. Picosecond pulse amplification by coherent wave mixing in silicon. Phys. Rev. (A), 1987, 35(11): 4673～4678

[7] I. C. Khoo, Ping Zhou, P. G. Lindquist et al.. Quantitative analysis of picosecond transient multiwave-mixing-mediated beam-amplification effect in silicon. Phy. Rev. (A), 1990, 41(1): 408～413

[8] G. C. Valley, J. Dubrad, A. L. Smirl. Theory of high gain transient energy transfer in GaAs and Si. IEEE J. Quant. Electron., 1990, QE-26(6): 1058～1066

[9] A. Penzkofer. Passive Q-switching and mode-locking for the generation of nanosecond to femtosecond pulses. Appl. Phys. (B), 1988,46(1): 43～60

[10] I. C. Khoo, R. Normandin. Nanosecond laser amplification via degenerate multiwave mixing in silicon. Appl. Phys. Lett., 1988, 52(7): 525～527