Fig. 1. Dependence of on the crystal orientation angle for ZnSe crystal at ^[32]线偏振光激发下ZnSe晶体中晶体取向角 依赖的双光子吸收系数 ^[32]

Fig. 2. [in Chinese]

Fig. 3. Far-field intensity patterns with polarization distributions of radially polarized beams for anisotropic Kerr media with different values of and ^[28]在不同 和 下，径向偏振光经过各向异性非线性克尔介质后远场的光强和偏振态分布^[28]

Fig. 4. Far-field intensity patterns with polarization distributions of hybridly polarized beams for isotropic Kerr media with different values of and ^[27]在不同 和 下，杂化偏振光经过各向同性非线性克尔介质后远场的光强和偏振态分布^[27]

Fig. 5. Far-field intensity patterns and spin angular momentumdistributions with polarization distributions of hybridly polarized beams through anisotropic Kerr nonlinearities for different crystal orientation angles ^[29]在不同晶体取向角 下，杂化偏振光经各向异性非线性克尔介质后远场光强分布、自旋角动量及偏振态分布^[29]

Fig. 6. [in Chinese]

Fig. 7. [in Chinese]

Fig. 8. [in Chinese]

Fig. 9. [in Chinese]

Fig. 10. Collapsing behaviors of (the first row) hybrid polarized beam and (the second row) radially polarized beam with random noises propagating in isotropic Kerr media. The four columns (from left to right) correspond to four propagation distances in units of diffraction length ( , 0.12, 0.24, and 0.36). The distributions of state of polarization are also shown in the first column^[45]具有随机噪声的杂化偏振光（第一行）和径向偏振光（第二行）在各向同性克尔介质中的塌缩行为。这四列（从左到右）依次对应以衍射长度为单位的四个传播距离（ , 0.12, 0.24, 和0.36）。第一列还给出了偏振态分布^[45]

Fig. 11. [in Chinese]