Fig. 1. CGI system for penetrating scattering media

Fig. 2. Measurement matrix projected in PPC method

Fig. 3. Fitting of the first 20 light intensity values with PPC method. (a) Light intensity with slow change of concentration of scattering media; (b) light intensity with steep change of concentration of scattering media

Fig. 4. Change of factor α in the dynamic scattering media

Fig. 5. Intensity measurements after scattering media in different states. (a) Through static scattering media; (b) through dynamic scattering media

Fig. 6. Reconstructed images through different scattering media. (a) Through static scattering media; (b) through dynamic scattering media

Fig. 7. Image restoration based on the PPC method. (a) Corrected measurements using PPC method; (b) reconstructed image using PPC method

Fig. 8. Comparison of reconstructed images with different measurement times. (a) 1000; (b) 3000; (c) 5000; (d) 8000

Fig. 9. PSNR values under PPC and TVAL3 versus the total measurement times

Fig. 10. Reconstructed images under multiplexing noise with different variances. (a) Reconstructed images by PPC method; (b) reconstructed images by TVAL3 method

Fig. 11. Reconstructed images under additive noise with different fluctuation levels. (a) Reconstructed images by PPC method; (b) reconstructed images by TVAL3 method