• Laser & Optoelectronics Progress
  • Vol. 59, Issue 6, 0617031 (2022)
Weitong Li1, Haolin Wang1, Kang Li1, Guohua Geng1, Mingquan Zhou2, and Xin Cao1、*
Author Affiliations
  • 1School of Information Science & Technology, Northwest University, Xi'an , Shaanxi 710127, China
  • 2College of Information Science and Technology, Beijing Normal University, Beijing 100875, China
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    DOI: 10.3788/LOP202259.0617031 Cite this Article Set citation alerts
    Weitong Li, Haolin Wang, Kang Li, Guohua Geng, Mingquan Zhou, Xin Cao. Local-Connection-Network-Based Reconstruction Method for Cerenkov Luminescence Tomography[J]. Laser & Optoelectronics Progress, 2022, 59(6): 0617031 Copy Citation Text show less
    FES-LCN structure
    Fig. 1. FES-LCN structure
    Research object of inhomogeneous cylinder simulation experiment. (a) Inhomogeneous cylinder model; (b) example of grid model of inhomogeneous cylinder; (c) example of forward simulation result of inhomogeneous cylinder
    Fig. 2. Research object of inhomogeneous cylinder simulation experiment. (a) Inhomogeneous cylinder model; (b) example of grid model of inhomogeneous cylinder; (c) example of forward simulation result of inhomogeneous cylinder
    Reconstructed results in inhomogeneous cylinder simulation experiment with single light source. (a) Stereogram reconstructed by IVTCG; (b) stereogram reconstructed by MFCNN; (c) stereogram reconstructed by FES-LCN; (d) two-dimensional section of reconstructed result for IVTCG; (e) two-dimensional section of reconstructed result for MFCNN; (f) two-dimensional section of reconstructed result for FES-LCN
    Fig. 3. Reconstructed results in inhomogeneous cylinder simulation experiment with single light source. (a) Stereogram reconstructed by IVTCG; (b) stereogram reconstructed by MFCNN; (c) stereogram reconstructed by FES-LCN; (d) two-dimensional section of reconstructed result for IVTCG; (e) two-dimensional section of reconstructed result for MFCNN; (f) two-dimensional section of reconstructed result for FES-LCN
    Reconstruction results in inhomogeneous cylinder simulation experiment with dual light source. (a) Stereogram reconstructed by IVTCG; (b) stereogram reconstructed by MFCNN; (c) stereogram reconstructed by FES-LCN; (d) two-dimensional section of reconstructed result for IVTCG; (e) two-dimensional section of reconstructed result for MFCNN; (f) two-dimensional section of reconstructed result for FES-LCN
    Fig. 4. Reconstruction results in inhomogeneous cylinder simulation experiment with dual light source. (a) Stereogram reconstructed by IVTCG; (b) stereogram reconstructed by MFCNN; (c) stereogram reconstructed by FES-LCN; (d) two-dimensional section of reconstructed result for IVTCG; (e) two-dimensional section of reconstructed result for MFCNN; (f) two-dimensional section of reconstructed result for FES-LCN
    Research object of digital mouse simulation experiment. (a) Digital mouse model; (b) example of grid model of digital mouse; (c) example of forward simulation result of digital mouse
    Fig. 5. Research object of digital mouse simulation experiment. (a) Digital mouse model; (b) example of grid model of digital mouse; (c) example of forward simulation result of digital mouse
    Reconstruction results in digital mouse simulation experiment with single light source. (a) Stereogram reconstructed by IVTCG; (b) stereogram reconstructed by MFCNN; (c) stereogram reconstructed by FES-LCN; (d) two-dimensional section of reconstructed result for IVTCG; (e) two-dimensional section of reconstructed result for MFCNN; (f) two-dimensional section of reconstructed result for FES-LCN
    Fig. 6. Reconstruction results in digital mouse simulation experiment with single light source. (a) Stereogram reconstructed by IVTCG; (b) stereogram reconstructed by MFCNN; (c) stereogram reconstructed by FES-LCN; (d) two-dimensional section of reconstructed result for IVTCG; (e) two-dimensional section of reconstructed result for MFCNN; (f) two-dimensional section of reconstructed result for FES-LCN
    Reconstruction results in digital mouse simulation experiment with dual light source. (a) Stereogram reconstructed by IVTCG; (b) stereogram reconstructed by MFCNN; (c) stereogram reconstructed by FES-LCN; (d) two-dimensional section of reconstructed result for IVTCG; (e) two-dimensional section of reconstructed result for MFCNN; (f) two-dimensional section of reconstructed result for FES-LCN
    Fig. 7. Reconstruction results in digital mouse simulation experiment with dual light source. (a) Stereogram reconstructed by IVTCG; (b) stereogram reconstructed by MFCNN; (c) stereogram reconstructed by FES-LCN; (d) two-dimensional section of reconstructed result for IVTCG; (e) two-dimensional section of reconstructed result for MFCNN; (f) two-dimensional section of reconstructed result for FES-LCN
    Materialμax /mm-1μsx /mm-1
    Muscle0.005210.8
    Heart0.00836.733
    Lung0.013319.7
    Liver0.03297.0
    Bone0.006060.09
    Table 1. Optical parameters of inhomogeneous cylinder
    MethodCoordinate of the center of reconstructed light sourceCoordinate of the point with maximum energyECELRTV
    IVTCG(-1.65,3.18,10.87)(-1.60,2.95,11.01)0.6820.6030.57
    MFCNN(-1.12,2.92,11.08)(-1.60,2.95,11.01)0.1710.6031.23
    FES-LCN(-1.12,2.92,11.08)(-0.87,3.45,11.05)0.1710.4690.68
    Table 2. Results of three reconstruction methods in inhomogeneous cylinder simulation experiment with single light source
    MethodCoordinate of center of reconstructed light sourceCoordinate of the point with maximum energyECELRTV
    IVTCG

    (-5.61,2.74,8.12)

    (-3.02,2.91,9.60)

    (-4.31,3.20,8.62)

    (-3.37,2.87,9.09)

    1.4722.4291.52
    MFCNN

    (-5,65,2.85,8.08)

    (-1.07,2.95,10.79)

    (-5.48,2.35,8.26)

    (-1.6,2.95,11.01)

    0.3090.7351.06
    FES-LCN

    (-5,65,2.85,8.08)

    (-1.07,2.95,10.79)

    (-5.48,2.35,8.26)

    (-0.87,3.45,11.05)

    0.3090.6681.00
    Table 3. Results of three reconstruction methods in inhomogeneous cylinder simulation experiment with dual light source
    MethodCoordinate of the center of reconstructed light sourceCoordinate of the point with maximum energyECELRTV
    IVTCG(18.89,7.98,19.24)(19.40,8.36,19.15)1.6721.0810.43
    MFCNN(18.58,7.21,19.23)(18.14,7.18,18.61)0.3460.9811
    FES-LCN(18.58,7.21,19.23)(17.97,6.35,19.35)0.3450.8521
    Table 4. Results of three reconstruction methods in digital mouse simulation experiment with single light source
    MethodCoordinate of the center of reconstructed light sourceCoordinate of the point with maximum energyECELRTV
    IVTCG

    (18.46,11.79,14.67)

    (17.98,13.25,22.16)

    (18.46,11.79,14.67)

    (18.21,13.05,21.68)

    0.9161.0650.49
    MFCNN

    (18.42,11.39,15.42)

    (18.92,14.98,22.96)

    (18.28,10.69,22.96)

    (18.72,14.05,23.11)

    0.6100.8821.54
    FES-LCN

    (18.42,11.39,15.42)

    (18.92,14.98,22.96)

    (18.28,10.69,22.96)

    (18.08,14.44,22.36)

    0.6100.7061.53
    Table 5. Results of three reconstruction methods in digital mouse simulation experiment with dual light source
    Weitong Li, Haolin Wang, Kang Li, Guohua Geng, Mingquan Zhou, Xin Cao. Local-Connection-Network-Based Reconstruction Method for Cerenkov Luminescence Tomography[J]. Laser & Optoelectronics Progress, 2022, 59(6): 0617031
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