• Chinese Optics Letters
  • Vol. 13, Issue Suppl., S21405 (2015)
Dongzhou Zhong
Author Affiliations
  • School of Information Engineering, Wuyi University, Jiangmen 529020, China
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    DOI: 10.3788/COL201513.S21405 Cite this Article Set citation alerts
    Dongzhou Zhong. Control of the polarization switching and the nonlinear dynamic behaviors of vertical cavity surface-emitting lasers with external optical injection[J]. Chinese Optics Letters, 2015, 13(Suppl.): S21405 Copy Citation Text show less
    Schematic of the control scheme for the PS and the NDBs of optically injected VCSEL.
    Fig. 1. Schematic of the control scheme for the PS and the NDBs of optically injected VCSEL.
    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. 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=10ns1, and E02=0kV/mm. Blue-line: μM=1.048; red-line: μM=1.048; green-line: μM=1.1.
    PS law of the output light from S-VCSEL2 in one change period of the applied electric field E01, when μM=1.048.
    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.
    PS law of the output light from S-VCSEL2 in one change period of the applied electric field E01, when μM=1.1.
    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.
    PS law of the output light from S-VCSEL2 in one change period of the applied electric field E01, when μM=1.18.
    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.
    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. 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=10ns1, and E02=0kV/mm. Blue-line: μM=1.048; red-line: μM=1.048; green-line: μM=1.1.
    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. 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=10ns1, and E02=0kV/mm. Here, blue-line: x-LP; red-line: y-LP. E0= (a) 0, (b) 0.6849, (c) 1.326, and (d) 1.474kV/mm.
    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.
    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=10ns1, and E02=0kV/mm. Here, blue-line: x-LP; red-line: y-LP. E0= (a) 0, (b) 0.6849, (c) 1.326, and (d) 1.474kV/mm.
    Dongzhou Zhong. Control of the polarization switching and the nonlinear dynamic behaviors of vertical cavity surface-emitting lasers with external optical injection[J]. Chinese Optics Letters, 2015, 13(Suppl.): S21405
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