• Infrared and Laser Engineering
  • Vol. 51, Issue 3, 20210373 (2022)
Dekui Li1, Chenxiang Xu1, Bing Lin1, Kai Guo1, Ning Zhang2, Jun Gao1, and Zhongyi Guo1
Author Affiliations
  • 1School of Computer and Information, Hefei University of Technology, Hefei 230009, China
  • 2Beijing Electro-Mechanical Engineering Institute, Beijing 100074, China
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    DOI: 10.3788/IRLA20210373 Cite this Article
    Dekui Li, Chenxiang Xu, Bing Lin, Kai Guo, Ning Zhang, Jun Gao, Zhongyi Guo. Research progress on theory and applications of index of polarization purities[J]. Infrared and Laser Engineering, 2022, 51(3): 20210373 Copy Citation Text show less
    IPPs’ feasible region
    Fig. 1. IPPs’ feasible region
    (a) , , varying with the proportion of small particles in the purity space (backward detection); (b) of scattering medium as a function of the proportion of small particles (forward detection); (c) , , varying with different mean values for standard deviation of 0.01 μm (backward detection); (d) , , varying with different mean values for standard deviation of 1.05 μm (backward detection)(a) 、 、随大小微粒混合体积比的变化(后向探测);(b)大小微粒混合体积比对散射介质的退偏指数的影响(前向探测);(c)粒子标准差为0.01 μm时,、 、 随粒子均值的变化(后向探测);(d) 粒子标准差为1.05 μm时,、 、 随粒子均值的变化(后向探测)
    Fig. 2. (a) , , varying with the proportion of small particles in the purity space (backward detection); (b) of scattering medium as a function of the proportion of small particles (forward detection); (c) , , varying with different mean values for standard deviation of 0.01 μm (backward detection); (d) , , varying with different mean values for standard deviation of 1.05 μm (backward detection) (a) 、 、 随大小微粒混合体积比的变化(后向探测);(b)大小微粒混合体积比对散射介质的退偏指数 的影响(前向探测);(c)粒子标准差为0.01 μm时, 、 、 随粒子均值的变化(后向探测);(d) 粒子标准差为1.05 μm时, 、 、 随粒子均值的变化(后向探测)
    Polarization analysis of leaf. (a) Intensity; (b) ; (c) ; (d) –; (e) Linear retardance δ and (f) Pseudo-colored image of linear retardance植物叶子的偏振分析。(a) 强度;(b) ;(c) ;(d) -;(e) δ线性延迟;(f) 线性延迟的伪彩色图像
    Fig. 3. Polarization analysis of leaf. (a) Intensity; (b) ; (c) ; (d) – ; (e) Linear retardance δ and (f) Pseudo-colored image of linear retardance 植物叶子的偏振分析。(a) 强度;(b) ;(c) ;(d) - ;(e) δ线性延迟;(f) 线性延迟的伪彩色图像
    Pseudo-colored image of different bases and weights. (a) α1 = 3, α2 = 1 and α3 = 1 of Eq. (11); (b) α1 = 2, α2 = 2 and α3 = 1 of Eq. (12)
    Fig. 4. Pseudo-colored image of different bases and weights. (a) α1 = 3, α2 = 1 and α3 = 1 of Eq. (11); (b) α1 = 2, α2 = 2 and α3 = 1 of Eq. (12)
    P1 and DoP varying with GC (forward scatter)
    Fig. 5. P1 and DoP varying with GC (forward scatter)
    [in Chinese]
    Fig. 6. [in Chinese]
    Space distribation and frequency distribution histogram of of detecting board with four kinds of GCs四种不同GC溶液下探测板(200×200)的空间分布和的频率分布直方图
    Fig. 6. Space distribation and frequency distribution histogram of of detecting board with four kinds of GCs 四种不同GC溶液下探测板(200×200)的 空间分布和 的频率分布直方图
    (a) Model of refraction and reflection; (b) Top view of upper hemisphere
    Fig. 7. (a) Model of refraction and reflection; (b) Top view of upper hemisphere
    Distributions of , , corresponding to different incident angles. (a) Samples as Cu, Au, Al; (b) Samples as Al, Al2O3随着入射角的变化,不同目标的、 、在纯度空间下的分布。(a) Cu、Au、Al;(b) Al、Al2O3
    Fig. 8. Distributions of , , corresponding to different incident angles. (a) Samples as Cu, Au, Al; (b) Samples as Al, Al2O3随着入射角的变化,不同目标的 、 、 在纯度空间下的分布。(a) Cu、Au、Al;(b) Al、Al2O3
    , , of each grid in the upper hemisphere varying with the incident angles (Cu)、、上半球的每个网格分布随入射角的变化(Cu)
    Fig. 9. , , of each grid in the upper hemisphere varying with the incident angles (Cu) 、 、 上半球的每个网格分布随入射角的变化(Cu)
    Dekui Li, Chenxiang Xu, Bing Lin, Kai Guo, Ning Zhang, Jun Gao, Zhongyi Guo. Research progress on theory and applications of index of polarization purities[J]. Infrared and Laser Engineering, 2022, 51(3): 20210373
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