• Journal of Infrared and Millimeter Waves
  • Vol. 40, Issue 5, 685 (2021)
Shi-Jie LIU1、2, Chun-Lai LI1、*, Rui XU1, Guo-Liang TANG1、2, Bing WU1、2, Yan XU1、2、4, and Jian-Yu WANG1、2、3、**
Author Affiliations
  • 1Key Laboratory of Space Active Opto-Electronics Technology,Shanghai Institute of Technical Physics,Chinese Academy of Sciences,Shanghai 200083,China
  • 2University of Chinese Academy of Sciences,Beijing 100049,China
  • 3Hangzhou Institute for Advanced Study,University of Chinese Academy of Sciences,Hangzhou,310024China
  • 4School of Information Science&Techno1ogy,ShanghaiTech University,Shanghai 200020,China
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    DOI: 10.11972/j.issn.1001-9014.2021.05.016 Cite this Article
    Shi-Jie LIU, Chun-Lai LI, Rui XU, Guo-Liang TANG, Bing WU, Yan XU, Jian-Yu WANG. High-precision algorithm for restoration of spectral imaging based on joint solution of double sparse domains[J]. Journal of Infrared and Millimeter Waves, 2021, 40(5): 685 Copy Citation Text show less
    Spectrum data can be divided into contour and details
    Fig. 1. Spectrum data can be divided into contour and details
    igh and low frequency distribution of corresponding signals when σ is 10,25,250
    Fig. 2. igh and low frequency distribution of corresponding signals when σ is 10,25,250
    Recovery results of different sampling rates under different sparsity constraints (a) Sampling rate: 40%, σ: 10, (b) Sampling rate: 40%, σ: 25, (c) Sampling rate: 40%, σ: 250,(d) Sampling rate: 80%, σ: 10, (e) Sampling rate: 80%, σ: 25, (f) Sampling rate: 80%, σ: 250
    Fig. 3. Recovery results of different sampling rates under different sparsity constraints (a) Sampling rate: 40%, σ: 10, (b) Sampling rate: 40%, σ: 25, (c) Sampling rate: 40%, σ: 250,(d) Sampling rate: 80%, σ: 10, (e) Sampling rate: 80%, σ: 25, (f) Sampling rate: 80%, σ: 250
    Test results on 500 samples (a) (b): Comparison of recovery accuracy at different sampling rates (σ: 15) ,(c) (d):σ’s impact on recovery accuracy (Sampling rate: 40%)
    Fig. 4. Test results on 500 samples (a) (b): Comparison of recovery accuracy at different sampling rates (σ: 15) ,(c) (d):σ’s impact on recovery accuracy (Sampling rate: 40%)
    Information distribution of carnauba wax spectrum corresponding to different sparse transforms(a)Distribution of different sparse transform coefficients,(b):Distribution during signal reconstruction at σ=10,(c)Distribution during signal reconstruction at σ=100
    Fig. 5. Information distribution of carnauba wax spectrum corresponding to different sparse transforms(a)Distribution of different sparse transform coefficients,(b):Distribution during signal reconstruction at σ=10,(c)Distribution during signal reconstruction at σ=100
    Effect of σ on the recovery results of different sparse decompositions. (a) (b) at a sampling rate of 40%,(c) (d) at a sampling rate of 80%
    Fig. 6. Effect of σ on the recovery results of different sparse decompositions. (a) (b) at a sampling rate of 40%,(c) (d) at a sampling rate of 80%
    Effect of σ on recovery speed of different sparse decompositions. (a) (b) at a sampling rate of 40%,(c) (d) at a sampling rate of 80%
    Fig. 7. Effect of σ on recovery speed of different sparse decompositions. (a) (b) at a sampling rate of 40%,(c) (d) at a sampling rate of 80%
    Laboratory verification equipment and verification results(a)CASSI system,(b)recovered true color image by 80% sampling,(c)PHI imaging results,(d)~(g)Recovered results by two algorithms under 20%,40%,80% and 100%sampling
    Fig. 8. Laboratory verification equipment and verification results(a)CASSI system,(b)recovered true color image by 80% sampling,(c)PHI imaging results,(d)~(g)Recovered results by two algorithms under 20%,40%,80% and 100%sampling

    输入:y,Φ

    输出:x

    1:设置σ,求解:
    2:设置ζ,求解:其中:yh=y-ylyl=Φx̂l=ΦΨθ̂l =Θθ̂l
    3、返回: ,其中:
    Table 1. Method Based on Joint of Double Sparse Domains
    算法名称采样率DCTDWT(db4)DWT(sysm4)DWT(coif4)Average
    SAMGSAMSAMGSAMSAMGSAMSAMGSAMSAMGSAM
    OMP20%0.6540.4790.6630.4820.6770.5790.6640.4450.6650.496
    40%0.7230.5740.7330.5970.7340.6770.7330.5540.7380.600
    80%0.9180.7920.9260.8230.9210.8930.8830.8070.9120.829
    IRLS20%0.6620.4810.6700.5830.6800.4930.6310.4430.6140.500
    40%0.7160.5920.7260.6970.7340.6070.7000.5610.7190.614
    80%0.8980.7720.9020.8790.9200.8820.8580.7470.8950.820
    TwIST20%0.5960.5560.5860.5770.6220.5720.5830.5440.5970.562
    40%0.6680.6470.6790.6280.7180.6720.6510.6330.6790.645
    80%0.8430.8300.8810.8660.9030.8500.8320.8270.8650.843
    GPSR20%0.6240.5040.6360.5440.6240.4820.6150.4820.6250.503
    40%0.6970.5470.7170.5830.6990.5470.6860.5330.7000.553
    80%0.7700.6920.7980.7520.7910.6320.7640.6840.7810.690

    JDSD1

    (OMP+IRLS)

    20%0.8510.5610.8870.8650.8910.6610.8890.8750.8800.741
    40%0.8950.7120.9320.9190.9420.8800.9410.9000.9280.853
    80%0.9620.8710.9420.9320.9520.8920.9630.9210.9550.904

    JDSD2

    (OMP+TwIST)

    20%0.8560.6630.8630.6670.7560.6630.7560.5930.8080.647
    40%0.9320.7520.9410.7640.8320.7320.8720.7920.8940.760
    80%0.9720.8910.9800.9230.8820.8790.9420.8940.9440.897

    JDSD3

    (OMP+ GPSR)

    20%0.8310.5610.8270.6610.7310.5410.6610.5910.7620.589
    40%0.8650.7000.8530.7790.8650.7650.7650.7240.8370.742
    80%0.9420.8470.9360.9070.9020.8370.9020.8770.9210.891
    Table 2. Comparison of JDSD algorithm recovery results of different combinations
    Shi-Jie LIU, Chun-Lai LI, Rui XU, Guo-Liang TANG, Bing WU, Yan XU, Jian-Yu WANG. High-precision algorithm for restoration of spectral imaging based on joint solution of double sparse domains[J]. Journal of Infrared and Millimeter Waves, 2021, 40(5): 685
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