• Photonics Research
  • Vol. 10, Issue 3, 758 (2022)
Li Song and Edmund Y. Lam*
Author Affiliations
  • Department of Electrical and Electronic Engineering, The University of Hong Kong, Pokfulam, Hong Kong, China
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    DOI: 10.1364/PRJ.447862 Cite this Article Set citation alerts
    Li Song, Edmund Y. Lam. Fast and robust phase retrieval for masked coherent diffractive imaging[J]. Photonics Research, 2022, 10(3): 758 Copy Citation Text show less
    Typical masked CDI: in situ CDI setup [31].
    Fig. 1. Typical masked CDI: in situ CDI setup [31].
    Imaging results of the Pb growth experiment (amplitude reconstructions). (a)–(f), (m)–(r) ADMM phase retrieval results for No. 1–12 diffraction patterns; (g)–(l), (s)–(x) phase retrieval results for No. 1–12 diffraction patterns using the baseline method, respectively.
    Fig. 2. Imaging results of the Pb growth experiment (amplitude reconstructions). (a)–(f), (m)–(r) ADMM phase retrieval results for No. 1–12 diffraction patterns; (g)–(l), (s)–(x) phase retrieval results for No. 1–12 diffraction patterns using the baseline method, respectively.
    ADMM iterations for the Pb growth experiment (different colors for different diffraction patterns). Both converge quickly. (a) Error. (b) R-factor.
    Fig. 3. ADMM iterations for the Pb growth experiment (different colors for different diffraction patterns). Both converge quickly. (a) Error. (b) R-factor.
    Reconstructed object planes for No. 1 diffraction pattern. The main difference is the area outside the support. (a) ADMM. (b) Baseline.
    Fig. 4. Reconstructed object planes for No. 1 diffraction pattern. The main difference is the area outside the support. (a) ADMM. (b) Baseline.
    Imaging results of No. 1 diffraction pattern in the Pb growth experiment (amplitude reconstructions) using different phase retrieval methods. (a) Baseline. (b) ADMM. (c) WF. (d) TWF.
    Fig. 5. Imaging results of No. 1 diffraction pattern in the Pb growth experiment (amplitude reconstructions) using different phase retrieval methods. (a) Baseline. (b) ADMM. (c) WF. (d) TWF.
    ADMM iterations for the glioblastoma experiment (different colors for different diffraction patterns). (a) Error. (b) R-factor.
    Fig. 6. ADMM iterations for the glioblastoma experiment (different colors for different diffraction patterns). (a) Error. (b) R-factor.
    Imaging results of the glioblastoma experiment (phase reconstructions). (a)–(f), (m)–(r) ADMM phase retrieval results for No. 1–12 diffraction patterns; (g)–(l), (s)–(x) phase retrieval results for No. 1–12 diffraction patterns using the baseline method, respectively.
    Fig. 7. Imaging results of the glioblastoma experiment (phase reconstructions). (a)–(f), (m)–(r) ADMM phase retrieval results for No. 1–12 diffraction patterns; (g)–(l), (s)–(x) phase retrieval results for No. 1–12 diffraction patterns using the baseline method, respectively.
    Processing time in different experiments (unit: s). (a) Pb growth experiment. (b) Glioblastoma experiment.
    Fig. 8. Processing time in different experiments (unit: s). (a) Pb growth experiment. (b) Glioblastoma experiment.
    Phase retrieval results with single diffraction pattern. (a), (b) Baseline method and ADMM method for No. 10 diffraction pattern in the Pb growth experiment; (c), (d) baseline method and ADMM method for No. 7 diffraction pattern in the glioblastoma experiment, respectively.
    Fig. 9. Phase retrieval results with single diffraction pattern. (a), (b) Baseline method and ADMM method for No. 10 diffraction pattern in the Pb growth experiment; (c), (d) baseline method and ADMM method for No. 7 diffraction pattern in the glioblastoma experiment, respectively.
    No.123456
    PSNR (dB)31.032.533.534.734.734.1
    SSIM0.880.850.840.860.860.86
    No.789101112
    PSNR (dB)34.033.433.734.333.633.1
    SSIM0.850.840.860.860.860.86
    Table 1. Numerical Comparison between ADMM and Baseline Method for Pb Growth Experiment
    Input:o: captured diffraction pattern; L: probe; Wo,Wb: dynamic and static masks; r: known static pattern; R: regularization function; u^(0),ϕ(0),u(0),λ(0),μ(0): initial values; ρ, τ: penalty parameters; ϵtol: error tolerance.
    Output: optimal reconstructed image u*
    1: repeat
    2:  u^(k+1)=(ρLHFHFL+τWoHWo)1[ρ(FL)H(oϕ(k)λ(k))
    3:      +τWoH(u(k)+WoWbr+μ(k))];
    4:  ϕ(k+1)=Po(λ(k)+FLu^(k+1));
    5:  u(k+1)=proxRτ[Wo(u^(k+1)Wbrμ(k))];
    6:  λ(k+1)=λ(k)+FLu^(k+1)oϕ(k+1);
    7:  μ(k+1)=μ(k)+u(k+1)Wo(u^(k+1)Wbr).
    8: until(u(k+1)u(k)2u(k+1)2<ϵtol)
    Table 1. PnP-ADMM for Masked CDI
    No.123456
    ADMM0.5990.6010.5950.6420.8160.820
    Baseline0.8460.8220.8690.9401.3721.527
    No.789101112
    ADMM0.8180.8110.7790.7220.7050.648
    Baseline1.4851.4451.3971.3161.3651.378
    Table 2. Mean Total Variation Loss of Different Methods for Glioblastoma Experiment
    No.1234567
    ADMM0.390.380.370.370.380.370.37
    Baseline39.4140.7438.8039.1039.2938.9639.23
    No.89101112AvgVar
    ADMM0.370.360.370.360.370.377×105
    Baseline39.2439.1239.2438.8839.4539.290.25
    Table 3. Processing Time of Different Algorithms in Pb Growth Experiment (Unit: s)
    No.1234567
    ADMM0.350.340.340.330.330.340.33
    Baseline40.2539.9739.9340.6440.5640.1440.15
    No.89101112AvgVar
    ADMM0.340.340.340.340.340.342×105
    Baseline41.0939.7640.5640.0041.5040.380.27
    Table 4. Processing Time of Different Algorithms in Glioblastoma Experiment (Unit: s)
    Li Song, Edmund Y. Lam. Fast and robust phase retrieval for masked coherent diffractive imaging[J]. Photonics Research, 2022, 10(3): 758
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