In this paper we study the influence of the relative phase between .the probe and driving fields on propagation effect in an open Doppler broadening V-type three-level atomic system with spontaneously generated cohere...In this paper we study the influence of the relative phase between .the probe and driving fields on propagation effect in an open Doppler broadening V-type three-level atomic system with spontaneously generated coherence （SGC） by using the calculation resuk of the density matrix motion equations and the propagation equations of the driving and probe fields. It is shown that the relative phase （Ф） has remarkable periodical influence on the propagation effect, and the period is 2π. By selecting appropriate value of Ф, we can get larger lasing without inversion （LW1） gain and longer propagation distance in which gain exists, and hence obtain higher probe field （i.e. LWI） intensity. When Ф=π/2, the largest LWI gain and probe field intensity can be got. In addition, the atomic exit rate （γ0） and ratio （S） of the atomic injection rates also have a considerable modulation role on the phase-dependent propagation effect. In certain value range of Y0 （S）, LWI gain and probe field intensity increase with γ0 （S） increasing. In the open system, LWI gain and probe field intensity much larger than those in the corresponding closed system can be obtained.展开更多
基金supported by the National Natural Science Foundation of China(No.10875072)
文摘In this paper we study the influence of the relative phase between .the probe and driving fields on propagation effect in an open Doppler broadening V-type three-level atomic system with spontaneously generated coherence （SGC） by using the calculation resuk of the density matrix motion equations and the propagation equations of the driving and probe fields. It is shown that the relative phase （Ф） has remarkable periodical influence on the propagation effect, and the period is 2π. By selecting appropriate value of Ф, we can get larger lasing without inversion （LW1） gain and longer propagation distance in which gain exists, and hence obtain higher probe field （i.e. LWI） intensity. When Ф=π/2, the largest LWI gain and probe field intensity can be got. In addition, the atomic exit rate （γ0） and ratio （S） of the atomic injection rates also have a considerable modulation role on the phase-dependent propagation effect. In certain value range of Y0 （S）, LWI gain and probe field intensity increase with γ0 （S） increasing. In the open system, LWI gain and probe field intensity much larger than those in the corresponding closed system can be obtained.
