• Chinese Optics Letters
  • Vol. 15, Issue 10, 102801 (2017)
Guo Zhang1、2, Jianfeng Sun1、*, Yu Zhou1, Zhiyong Lu1, Guangyuan Li1、2, Guangyu Cai1、2, Mengmeng Xu1、2, Bo Zhang1、2, Chenzhe Lao1、2, Hongyu He1、2, and Liren Liu1
Author Affiliations
  • 1Key Laboratory of Space Laser Communication and Detection Technology, Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Science, Shanghai 201800, China
  • 2University of Chinese Academy of Sciences, Beijing 100049, China
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    DOI: 10.3788/COL201715.102801 Cite this Article Set citation alerts
    Guo Zhang, Jianfeng Sun, Yu Zhou, Zhiyong Lu, Guangyuan Li, Guangyu Cai, Mengmeng Xu, Bo Zhang, Chenzhe Lao, Hongyu He, Liren Liu. Imaging process and signal-to-noise ratio improvement of enhanced self-heterodyne synthetic aperture imaging ladar[J]. Chinese Optics Letters, 2017, 15(10): 102801 Copy Citation Text show less
    Structure of the enhanced self-heterodyne SAIL system. PBS: polarizing beam splitter; WP: wave plate.
    Fig. 1. Structure of the enhanced self-heterodyne SAIL system. PBS: polarizing beam splitter; WP: wave plate.
    Configuration to translate the wavefront using cylindrical lenses; x means the cylindrical lenses L1 and L2 are moving in the direction orthogonal to the direction of travel, y means the cylindrical lenses L3 and L4 are moving in the travel direction.
    Fig. 2. Configuration to translate the wavefront using cylindrical lenses; x means the cylindrical lenses L1 and L2 are moving in the direction orthogonal to the direction of travel, y means the cylindrical lenses L3 and L4 are moving in the travel direction.
    (a) Magnitude and (b) phase distributions of the focused image in the orthogonal direction of travel and (c) a 2D image focused subsequently in the travel direction for a 0.3 mm×0.3 mm point target. The distribution of the final image is (d) in orthogonal direction and (e) in the travel direction for a 0.3 mm×0.3 mm point target.
    Fig. 3. (a) Magnitude and (b) phase distributions of the focused image in the orthogonal direction of travel and (c) a 2D image focused subsequently in the travel direction for a 0.3mm×0.3mm point target. The distribution of the final image is (d) in orthogonal direction and (e) in the travel direction for a 0.3mm×0.3mm point target.
    (a), (b), and (c) are the final images for a 0.3 mm×0.3 mm point target at output power of 15 mW, 2 mW, and 750 μW of the optical fiber amplifier. (d), (e), and (f) are the distribution of the final image in the travel direction for a 0.3 mm×0.3 mm point target at the output powers of 15 mW, 2 mW, and 750 μW of the optical fiber amplifier.
    Fig. 4. (a), (b), and (c) are the final images for a 0.3mm×0.3mm point target at output power of 15 mW, 2 mW, and 750 μW of the optical fiber amplifier. (d), (e), and (f) are the distribution of the final image in the travel direction for a 0.3mm×0.3mm point target at the output powers of 15 mW, 2 mW, and 750 μW of the optical fiber amplifier.
    Self-heterodyne receiver in the down-looking SAIL.
    Fig. 5. Self-heterodyne receiver in the down-looking SAIL.
    (a), (b), and (c) are the final images for a 0.3 mm×0.3 mm point target in the down-looking SAIL at the output powers of 15 mW, 2 mW, and 750 μW of the optical fiber amplifier. (d), (e), and (f) are final images in the travel direction for a 0.3 mm×0.3 mm point target in the down-looking SAIL at the output powers of 15 mW, 2 mW, and 750 μW of the optical fiber amplifier.
    Fig. 6. (a), (b), and (c) are the final images for a 0.3mm×0.3mm point target in the down-looking SAIL at the output powers of 15 mW, 2 mW, and 750 μW of the optical fiber amplifier. (d), (e), and (f) are final images in the travel direction for a 0.3mm×0.3mm point target in the down-looking SAIL at the output powers of 15 mW, 2 mW, and 750 μW of the optical fiber amplifier.
    Output power of the optical fiber amplifierIntensity of point target IpIntensity of noise σpSNRp
    15 mW1127191124
    2 mW164115109
    750 μW364661
    Table 1. SNR of Point Target Final Image in Enhanced Self-heterodyne SAIL System
    Output power of the optical fiber amplifierIntensity of point target IpIntensity of noise σpSNRp
    15 mW375.283.8797
    2 mW61.592.3726
    750 μW15.52.466
    Table 2. SNR of Point Target Final Image in Down-looking SAIL
    Guo Zhang, Jianfeng Sun, Yu Zhou, Zhiyong Lu, Guangyuan Li, Guangyu Cai, Mengmeng Xu, Bo Zhang, Chenzhe Lao, Hongyu He, Liren Liu. Imaging process and signal-to-noise ratio improvement of enhanced self-heterodyne synthetic aperture imaging ladar[J]. Chinese Optics Letters, 2017, 15(10): 102801
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