[1] STOLER D, SALEH B, TEICH M C. Binomial states of the quantized radiation field[J]. Optica Acta, 1985, 32(3): 345355.
[2] DATTPLI G, GALLARDO J, TORRE A. Binomial states of the quantized radiation field: comment[J]. JOSA B, 1987, 4(2): 185191.
[3] FRANCO R L, COMPAGNO G, MESSINA A, et al. Singleshot generation and detection of a twophoton generalized binomial state in a cavity[J]. Physical Review A, 2006, 74(4): 58035806.
[4] FRANCO R L, COMPAGNO G, MESSINA A, et al. Efficient generation of Nphoton binomial states and their use in quantum gates in cavity QED[J]. Physics Letters A, 2010, 374(22): 22352242.
[5] HU Yaohua, FANG Maofa, JIANG Chunlei. Quantum properties of the binomial state field interacting with a cascade threelevel atom[J]. Chinese Journal of Quantum Electronics, 2006, 23(6): 843847.
[6] VERNA A, SHARMA N K, PATHAK A. Higher order antibunching in intermediate states[J]. Physics Letters A, 2008, 372(18): 55425551.
[7] HU Yaohua, FANG Maofa, LIAO Xiangping, et al. Quantum entanglement of the binomial field interacting with a cascade threelevel atom[J]. Acta Physica Sinica, 2006, 55(9): 46314637.
[8] IRISH E K, GEABANACLOCHE J, MARTIN I, et al. Dynamics of a twolevel system strongly coupled to a highfrequency quantum oscillator[J]. Physical Review B, 2006, 72(19): 195410.
[9] GUNTER G, ANAPPARA A A, HEES J, et al. Subcycle swithon of ultrastrong lightmatter interaction[J]. Nature, 2009, 458(12): 178181.
[10] JIA Fei, XIE Shuangyuan, YANG Yaping. Interaction of an atom with a field with varying frequency without rotatingwave approximation[J]. Acta Physica Sinica, 2006, 55(11): 58355841.
[11] GAMBETTA J, BLAIS A, SCHUSTER D I, et al. Qubitphoton interactions in a cavity: Measurementinduced dephasing and number splitting[J]. Physical Review A, 2006, 74(4): 042318.
[12] REN Xuezao, JIANG Daolai, CONG Honglu, et al. Exact calculations of the energy spectra and the dynamical properties of a twolevel system[J]. Acta Physica Sinica, 2009, 58(8): 53945399.
[13] REN Xuezao, LIAO Xu, HUANG Shuwen. Study of onedimensional Holstein polaron in infinite lattice[J]. Acta Physica Sinica, 2009, 58(4): 26802683.
[14] CONG Honglu, REN Xuezao, JIANG Daolai, et al. An exact solution of evolution of the field entropy in a system of threelevel cascade type atom interacting with singlemode coherent field[J]. Acta Physica Sinica, 2010, 59(5): 32213226.
[15] REN Xuezao, CONG Honglu, WANG Xuwen, et al. Quantum entanglement of the bimomial field interacting with a cascade threelevel atom beyond the rotating wave approximation[J]. Science in China Series G, 2011, 54(9): 16251630.
[16] CHEN Qinghu, ZHANG Yuyu, LIU Tao, et al. Numerically exact solution to the finitesize Dicke model[J]. Physical Review A, 2008, 78(5): 051801.
[17] LIU Tao, WANG Kelin, FENG Mang. Lower ground state due to counterrotating wave interaction in a trapped ion system[J]. Journal of Physics B, 2007, 40(11): 19671974.
[18] LIU Tao, ZHANG Yuyu, CHEN Qinghu, et al. LargeN scaling behavior of the groundstate energy, fidelity, and the order parameter in the dicke model[J]. Physical Review A, 2009, 80(2): 023801.
[19] LU Daoming. Squeezing effects of field with a tinevarying frequency in the multiphotonjaynescummings model[J]. Acta Photonica Sinica, 2009, 38(7): 18401845.
[20] MENG Xiangguo, WANG Jisuo. New even and odd nonlinear coherent states and their nonclassical properties[J]. Acta Physica Sinica, 2006, 56(4): 21542159.
[21] ZHANG WANjuan, WANG Zhiguo, Xie Shuangyuan, et al. Interaction of an atom with a squeezed field of timevarying frequency[J]. Acta Physica Sinica, 2007, 56(4): 21682174.
[22] WAN Lin, LIU Sumei, LIU Sanqiu. Influences of the virtual photon process on the squeezing effects of a singlemode light field in the TC model[J]. Acta Physica Sinica, 2002, 51(1): 8490.
[23] LIAO Xu, CONG Honglu, JIANG Daolai, et al. Influence of the field with varying frequency modulation on atomic population inversion in nonratatingwave approximation[J]. Acta Physica Sinica, 2010, 59(8): 55085513.