Fig. 1. Schematic of the control scheme for the PS and the NDBs of optically injected VCSEL.

Fig. 2. For different bias current μM of M-VCSEL, the dependence of the output PD2 of light from S-VCSEL2 with POI on the applied electric field E01, where μS=1.2, Kinj=10  ns−1, and E02=0  kV/mm. Blue-line: μM=1.048; red-line: μM=1.048; green-line: μM=1.1.

Fig. 3. PS law of the output light from S-VCSEL2 in one change period of the applied electric field E01, when μM=1.048.

Fig. 4. PS law of the output light from S-VCSEL2 in one change period of the applied electric field E01, when μM=1.1.

Fig. 5. PS law of the output light from S-VCSEL2 in one change period of the applied electric field E01, when μM=1.18.

Fig. 6. For different bias current μM of the M-VCSEL, the dependence of the output PD2 of light from S-VCSEL1 with OOI on the applied electric field E01, where μS=1.2, Kinj=10  ns−1, and E02=0  kV/mm. Blue-line: μM=1.048; red-line: μM=1.048; green-line: μM=1.1.

Fig. 7. Under different the applied electric field E01, the temporal traces of the light intensity of the output x- or y-LP mode component from S-VCSEL2 with POI when μS=1.2, μM=1.18, kinj=10  ns−1, and E02=0  kV/mm. Here, blue-line: x-LP; red-line: y-LP. E0= (a)  0 , (b) 0.6849, (c) 1.326 , and (d) 1.474  kV/mm.

Fig. 8. Under different the applied electric field E01, the temporal traces of the light intensity of the output x- or y-LP mode component from S-VCSEL1 with OOI when μS=1.2, μM=1.18, kinj=10  ns−1, and E02=0  kV/mm. Here, blue-line: x-LP; red-line: y-LP. E0= (a) 0  , (b) 0.6849 , (c) 1.326, and (d) 1.474  kV/mm.