[1] Jaynes E T, Cummings F W. Comparison of quantum and semiclassical radiation theories with application to beam maser [J]. Proc. IEEE., 1963, 51: 89.

[2] Tavis M, Cummings F W. Exact solution for an N-molecule-radiation-field Hamiltonian [J]. Phys. Rev., 1968,A170(2): 379-384.

[3] Agarwall G S, Narducci M, Apostolidis E. Effects of dispersion forces in optical resonance phenomena [J]. Opt.Commun., 1981, 36: 285.

[4] Griffin R D, Harris S M. Two-atom resonance fluorescence including the dipole-dipole interaction [J]. Phys. Rev.,1982, A25: 1528.

[5] Joshi A, Puri R R, Lawande S V. Effect of dipole interaction and phase-interrupting collisions on the collapseand-revival phonomenon in the Jaynes-Cummings model [J]. Phys. Rev., 1991, A44: 2135.

[9] Stoler D, Saleh B E A, Teich M C. Binomial states of the quantized radiation field [J]. Acta Opt., 1985, 32: 345.

[12] Fan H Y, Jing S C. Connection of a type pf q-deformed binomial state with q-spin coherent states [J]. Phys. Rev.,1994, A50(2): 1909.