[1] Xie F S,Chen M Y,Liu X Q. Two-mode squeezed vacuum field interacting non-resonantly with a Λ-type three-level atom. Acta Photonica Sinica,2004,33(1):118~121
[2] Liu S M. The interaction of two coupling atoms between a single-mode squeezed coherent state light field. Acta Photonica Sinica,2004,33(1) :113~117
[3] Liu J. Thermal entanglement in a two-level atom resonantly coupled to single-mode cavity system. Acta Photonica Sinica,2005,34(5) :789~792
[4] Mompart J,Corbalan R. Lasing without inversion. J Optics B : Quant and Semiclas Opt,2000,2 (3) : R4~27
[5] Dong P,Man W,Gao J Y. Probe amplification from Raman gain to inversionless gain. Phys Lett A,2000,265(1): 43~50
[6] Belyanin A. Inversionless lasing with self-generated driving field. PhysRev A,2001,64(1) 013814:1~11
[7] Kocharovskaya O,Matsko A B,Rostovtsev Y,et al. Lasing without inversion via decay-induced coherence. PhysRevA,2001,65(1)013803:1~7
[8] Fan X J,Liu C P,Tian S F,et al. Doppler-enhanced gain in an open ladder inversionless lasing system. J Modern Opt,2004,51(3): 399~407
[9] Fan X J,Liu C P,Tian S F,et al. Destabilization of the non-lasing solution in open three-level systems. J Modern Opt,2003,50(11) :1763~1771
[10] Zhu Y F,Mullins O C,Xiao M. Inversionless laser from a closed multilevel system. PhysRevA,1993,47(1) : 602~609
[11] Sargent M,Scully M O,Lamb W L. Laser Physics. New York: Addison-Wesley,1973.121~130
[12] Louisell W H. Quantum statistical properties of radiation. New York: Wiley,1973.517~526
[13] Gong S Q,Du S D,Li Y,et al. Coherence and decoherence effects on lasing with or without population inversion in a four-level atomic system. Chin J Lasers,1997,B6(6):527~532
[14] Xu H,Li J,Liu J,et al. The effects of phase fluctuation in an open V-type inversionless lasing system. Acta Photonica Sinica,2003,32 (3) : 370~374
[15] Gong S Q,Xu Z Z. The effect of phase fluctuation on absorption and dispersion in a V medium. Opt Commun,1995,115(3):65~70