中国激光, 2019, 46 (8): 0801009, 网络出版: 2019-08-13
基于共轭微腔和磁微腔耦合共振的多偏振态激光输出 
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Multiple-Polarization Laser Based on Coupling of Conjugated and Magnetic Microcavities
图 & 表
图 2. 当ρA=ρC=0时,+z方向入射特定波长处出射和反射的极化状态
Fig. 2. Polarization states of output and reflected lasers corresponding to special incident wavelength in +z incident direction for ρA=ρC=0
图 3. 当ρA=ρC=0时,Ex和Ey透射和反射光谱及相应的相位差Δφ。(a) Ex透射和反射光谱; (b) +z入射方向Ex和Ey透射和反射的相位差; (c)Ey透射和反射光谱;(d) -z入射方向Ex和Ey透射和反射的相位差
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
图 4. 当ρA=ρC=0时,结构在5个共振波长处对应的场分布
Fig. 4. Field distributions corresponding to five resonant wavelengths for ρA=ρC=0
图 5. 当ρ=0.0196时,+z方向入射光的Ex和 Ey透射和反射光谱及相应的相位差Δ?。(a) Ex谱;(b) Ey谱;(c)相位差
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
图 6. 当ρ=0.0356时,两个方向入射光的Ex和 Ey 透射和反射光谱及相应的相位差Δ?。(a) +z方向入射光的Ex谱;(b) -z方向入射光的Ex谱;(c) +z方向入射光的Ey谱;(d) +z方向入射光的Ey谱;(e) +z方向入射光的相位差;(f) -z方向入射光的相位差
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
图 7. ρ=0.0356时,+z方向入射光在特定波长处的出射和反射的极化状态Fig,7 Polarization states of output and reflected lasers corresponding to special incident wavelength along +z incident direction for ρ=0.0356
Fig. 7.
图 8. ρ=0.041时,两个方向入射光的Ex 和 Ey 透射和反射光谱及相应的相位差Δ?。(a) +z方向Ex 谱;(b) -z方向Ex谱;(c) +z方向Ey 谱;(d) -z方向Ey 谱;(e) +z方向相位差;(f) -z方向相位差
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
图 9. ρ=0.041时,特定波长处相反入射方向的出射光和反射光的偏振状态(实线表示沿+z方向入射,虚线表示沿-z方向入射)
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
图 10. 在图8的超强模式λ3处 沿+z方向入射条件下结构内部的场分布
Fig. 10. Field distribution inside structure along +z incident direction for ultra-intense mode at λ3 in Fig. 8
吴义恒, 李小雪, 方云团. 基于共轭微腔和磁微腔耦合共振的多偏振态激光输出[J]. 中国激光, 2019, 46(8): 0801009. 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.
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