很明显的是，在低泵浦能量的状态下，参数q的最大值集中在横坐标零的附近，

It is evident that, in a state of low pump energy, the maximum value of parameter q is concentrated near zero abscissa, shown in Figure 4.1. With increasing pump energy, gradually move closer to the peak value of q ± 1, 4, 5, 6 relative changes as shown in FIG. This phenomenon is demonstrated, with the change of pump energy, laser sideband undergone a transition from a glassy state to a random state

Obviously, in the low pump energy state, the maximum value of parameter q is concentrated near the horizontal coordinate stake, as shown in Figure 4.1. As the pump ingress energy increases, the peak of q gradually moves closer to .1, as shown in Figure 4, Figure 5, and the relative change in Figure 6. This phenomenon proves that with the change of pump energy, the side-band laser has undergone a change from random state to glass state.

Obviously, in the state of low pump energy, the maximum value of parameter q is concentrated near the abscissa zero, as shown in Figure 4.1. With the increase of pump energy, the peak value of Q gradually approaches ± 1, as shown in the relative changes of Fig. 4, FIG. 5 and Fig. 6. This phenomenon proves that the sideband laser undergoes a transition from random state to glass state with the change of pump energy<br>