[1] [1] T. Kimura, K. Otsuka, M. Saruwatari. Spatial hole-burning of effects in a Nd3+:YAG laser. IEEE J. Quant. Electron., 1971, QE-7(6): 225～230

[2] [2] C. T. Pike. Spatial hole burning in CW dye lasers. Opt. Commun., 1974, 10(10): 14～17

[3] [3] H. W. Sohroder, H. Dux, H. Welling. Single mode operation of CW dye lasers. Appl. Phys., 1975, 7(1): 21～28

[4] [4] I. V. Hertel, A. S. Stamatovic. Spatial hole burning and oligomode distance control in CW dye lasers. IEEE J. Quant. Electron., 1975, QE-11(5): 210～212

[5] [5] I. McMackin, C. Radzewicz, N. Beck et al.. Instabililies and chaos in a multimode, Standing-wave, CW dye laser. Phys. Rev. (A), 1988, 38(7): 820～832

[6] [6] J. J. Zoyhowski. Limits imposed by spatial hole burning on the single-mode operation of standing-wave laser cavities. Opt. Lett., 1990, 15(4): 431～433

[7] [7] L. W. Casperson. Laser power calculations: sources of error. Appl. Opt., 1980, 19(2): 422～434

[8] [8] J. J. Zayhowski. The effects of spatial hole burning and energy diffusion on the single-mode operation of standing-wave lasers. IEEE J. Quant. Electron., 1990, QE-26(12): 2052～2057

[9] [9] G. J. Kintz, T. Baer. Single-frequency operation in solid-state laser materials with short absorption depths. IEEE J. Quant. Electron., 1990, QE-26(9): 1457～1459

[10] [10] T. Y. Fan, R. L. Byer. Diode laser-pumped solid-state lasers. IEEE J. Quant. Electron., 1988, QE-24(6): 895～912