摘要
Based on the density operator＇s operator-sum representation recently obtained by Fan and Hu for a laser process （Opt. Commun., 2008, 281： 5571; Opt. Commun., 2009, 282： 932; Phys. Lett. B, 2008, 22： 2435）, we derive the evolution law of Wigner operator, the law is concisely expressed in T exp[-2T（ate-（k-g）t - a.）（ae-（k-g）t a）]; where g the normally ordered form A（a,a＊,t） = -T/π., and a are the cavity gain and the loss, respectively, and T - （a - g）（g-t-g - 2ge-2（k-g）t）-1. When 1 exp[-2（at a＊）（a a）] which is the initial Wigner operator. Using this t = O, A（a,a＊,t） →1/π , formalism the evolution law of Wigner functions in laser process can be directly obtained.
Based on the density operator＇s operator-sum representation recently obtained by Fan and Hu for a laser process （Opt. Commun., 2008, 281： 5571; Opt. Commun., 2009, 282： 932; Phys. Lett. B, 2008, 22： 2435）, we derive the evolution law of Wigner operator, the law is concisely expressed in T exp[-2T（ate-（k-g）t - a.）（ae-（k-g）t a）]; where g the normally ordered form A（a,a＊,t） = -T/π., and a are the cavity gain and the loss, respectively, and T - （a - g）（g-t-g - 2ge-2（k-g）t）-1. When 1 exp[-2（at a＊）（a a）] which is the initial Wigner operator. Using this t = O, A（a,a＊,t） →1/π , formalism the evolution law of Wigner functions in laser process can be directly obtained.
