[1] Jung P, Hnggi P. Dynamical system: A unified colored-noise approximation. Phys. Rev. (A), 1987, 35(10):4464～4466

[2] Lett P, Gage E C, Chyba T H. Colored-noise-induced first-order phase transition in a single-mode dye laser. Phys. Rev. (A), 1987, 35(2):746～751

[3] Aguado M, San Miguel M. Analysis of a dye-laser model including quantum noise. Phys. Rev. (A), 1988, 37(2):450～455

[4] Young M R, Singh S. Observation of the ‘Brownian motion' of the electric field in a laser. Phys. Rev. (A), 1987, 35(3):1453～1456

[5] Lin L, Cao L, Wu D. First-order-like transition for colored-noise saturation models of dye lasers. Phys. Rev. (A), 1993, 48(1):739～745

[6] Jia Y, Li J. Steady-state analysis of a bistable system with additive and multiplicative noises. Phys. Rev. (E), 1996, 53(6):5786～5792

[7] Mei D, Xie G, Cao L et al.. Mean first-passage time of a bistable kinetic model driven by cross-correlated noises. Phys. Rev. (E), 1999, 59(4):3880～3883

[8] Risken H. Fokker-Planck Equation. Berlin: Springer, 1984. 50～56

[9] Sancho J M, San Miguel M, Katz S L et al.. Analytical and numerical studies of multiplicative noise. Phys. Rev. (A), 1982, 26(3):1589～1609

[10] Sancho S M, San Miguel M. External non-white noise and nonequilibrium phase transitions. Z. Physik (B), 1980, 36(4):357～364

[12] Cao L, Wu D, Lin L. First-order-like transition for colored saturation models of dye lasers: Effects of quantum noise. Phys. Rev. (A), 1994, 49(1):506～516

[13] Gilmare R. Catastrophe Theory for Scientists and Engineers. New York: John Wiley & Sons, 1981. 58～64

[14] Imbo T, Pagnamenla A, Sukhatme U. Energy eigenstates of spherically symmetric potentials using the shifted 1/N expansion. Phys. Rev. (D), 1984, 29(8):1669～1681