Chinese Journal of Lasers, Volume. 46, Issue 8, 0801009(2019)
Multiple-Polarization Laser Based on Coupling of Conjugated and Magnetic Microcavities
Fig. 2. Polarization states of output and reflected lasers corresponding to special incident wavelength in +z incident direction for ρA=ρC=0
Fig. 3. Transmission andreflection spectra of Ex and Ey and corresponding phase difference Δφ for ρA=ρC= 0. (a) Transmission and reflection spectra of Ex; (b) phase difference between transmission and reflection spectra of Ex and Ey in +z incident direction; (c) transmission and reflection spectra of Ey; (d) phase difference between transmission and reflection spectra of Ex and Ey in -z incident direction
Fig. 4. Field distributions corresponding to five resonant wavelengths for ρA=ρC=0
Fig. 5. Transmission and reflection spectra of Ex and Ey and corresponding phase difference Δ? along+z incident direction for ρ=0.0196. (a) Spectra of Ex; (b) spectra of Ey; (c) phase difference Δφ
Fig. 6. Transmission and reflection spectra of Ex and Ey along two incident directions and corresponding phase difference Δ? for ρ=0.0356. (a) Spectra of Ex along +z incident direction; (b) spectra of Ex along -z incident direction; (c) spectra of Ey along +z incident direction; (d) spectra of Ey along -z incident direction; (e) phase difference along +z incident direction; (f) phase difference along -z incident direction
Fig. 8. Transmission and reflection spectra of Ex and Ey and corresponding phase difference Δ? in two incident directions for ρ=0.041 and. (a) Spectra of Ex in +z incident direction; (b) spectra of Ex in -z incident direction; (c) spectra of Ey in +z incident direction; (d) spectra of Ey in -z incident direction; (e) phase difference in +z incident direction; (f) phase difference in -z incident direction
Fig. 9. Polarization states of output and reflected lasers corresponding to special incident wavelength along +z (solid line) and -z (dashed line) incident directions for ρ=0.041
Fig. 10. Field distribution inside structure along +z incident direction for ultra-intense mode at λ3 in Fig. 8
Fig. 11. Polarization states of transmission (solid line) and reflection (dashed line) for λ3=1368.56 nm under non-conjugated matching condition
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Yiheng Wu, Xiaoxue Li, Yuntuan Fang. Multiple-Polarization Laser Based on Coupling of Conjugated and Magnetic Microcavities[J]. Chinese Journal of Lasers, 2019, 46(8): 0801009
Category: laser devices and laser physics
Received: Mar. 20, 2019
Accepted: Apr. 19, 2019
Published Online: Aug. 13, 2019
The Author Email: Fang Yuntuan (fang_yt1965@sina.com)