Figure 1

(a) Stationary response functions of the driven polariton mode ($\mathbf{k}=0$) at different values of detuning $D$ of pump frequency from the lower polariton branch resonance. (b) Boundary of instability area of the stationary solution at $D=0.3$ meV with respect to fluctuations with various wave numbers $k_x$. Bifurcation points $[I_{1,2}{,\left(V\right|\mathcal{P}|}^2{)}_{1,2}]$ at $D=0.3$ meV, calculated with allowance made for possible breakup of the driven mode, are denoted by $•$; bifurcation points of the strictly one-mode solution are indicated by empty markers $\circ$.Reuse & Permissions

Figure 2

(a) Chosen time dependence of perturbation of exciton energy. (b) Calculated time dependence of cavity transmission intensity.Reuse & Permissions

Figure 3

“Instanteneous” response functions of the driven polariton mode $(\mathbf{k}=0)$ determined by different exciton energy values. Time points $t_1,t_2,...,t_7$ are shown in Fig. 2a. Heavy vertical line indicates the given pump intensity. Values $V|{\mathcal{P}}_0{|}^2$ expected in the stationary approximation and thus corresponding to the attractors of phase trajectory are indicated by empty markers ($\circ$). Dark markers ($•$) indicate actual [i.e., obtained by direct solution of multimode evolution equations (1) and (2)] values ${V\left|\mathcal{P}(\mathbf{k}=0,t)\right|}^2$ in chosen points of time. Horizontal dashed lines limit the instability areas of stationary solutions (also calculated in the multimode approximation).Reuse & Permissions

Figure 4

The dependencies of the time-averaged transmission intensities on the mean values $\langle \mathcal{A}\rangle$ of amplitudes of sequential strain pulses, for some different values of the variance ${\sigma }_{\mathcal{A}}^2$.Reuse & Permissions