• Acta Optica Sinica
  • Vol. 40, Issue 17, 1705001 (2020)
Chengcheng Chang1、2、3, Xingchen Pan1、2, Hua Tao1、2, Cheng Liu1、2、*, and Jianqiang Zhu1、2
Author Affiliations
  • 1National Laboratory on High Power Laser and Physics, Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Shanghai 201800, China
  • 2National Laboratory on High Power Laser and Physics, China Academy of Engineering Physics, Chinese Academy of Sciences, Shanghai 201800, China
  • 3University of Chinese Academy of Science, Beijing 100049, China
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    DOI: 10.3788/AOS202040.1705001 Cite this Article Set citation alerts
    Chengcheng Chang, Xingchen Pan, Hua Tao, Cheng Liu, Jianqiang Zhu. Reconstruction Algorithm for Ptychographic Iterative Engine with Highly Tilted Illumination[J]. Acta Optica Sinica, 2020, 40(17): 1705001 Copy Citation Text show less
    Schematic diagram of PIE with highly tilted illumination. (a) Optical path schematic; (b) flowchart of the algorithm
    Fig. 1. Schematic diagram of PIE with highly tilted illumination. (a) Optical path schematic; (b) flowchart of the algorithm
    Diffraction patterns with different incident angles. (a) Diffraction pattern calculated by spherical wave integration based on Huygens-Fresnel principle with large incident angle; (b) diffraction pattern calculated by the revised angular spectrum with the same incident angle; (c) diffraction pattern when the incident angle is 3°; (d) diffraction pattern when the incident angle is 0°
    Fig. 2. Diffraction patterns with different incident angles. (a) Diffraction pattern calculated by spherical wave integration based on Huygens-Fresnel principle with large incident angle; (b) diffraction pattern calculated by the revised angular spectrum with the same incident angle; (c) diffraction pattern when the incident angle is 3°; (d) diffraction pattern when the incident angle is 0°
    Simulated initial value. (a) Amplitude of specimen; (b) phase of specimen; (c) amplitude of probe light; (d)phase of probe light
    Fig. 3. Simulated initial value. (a) Amplitude of specimen; (b) phase of specimen; (c) amplitude of probe light; (d)phase of probe light
    Representative 9 diffraction patterns of dataset
    Fig. 4. Representative 9 diffraction patterns of dataset
    Reconstructed results based on general ePIE algorithm with highly tilted illumination after 500 iterations. (a) Amplitude of specimen; (b) phase of specimen; (c) amplitude of probe light; (d) phase of probe light
    Fig. 5. Reconstructed results based on general ePIE algorithm with highly tilted illumination after 500 iterations. (a) Amplitude of specimen; (b) phase of specimen; (c) amplitude of probe light; (d) phase of probe light
    Reconstructed results based on revised angular spectrum and ePIE after 500 iterations. (a) Amplitude of specimen; (b) phase of specimen; (c) amplitude of probe light; (d) phase of probe light
    Fig. 6. Reconstructed results based on revised angular spectrum and ePIE after 500 iterations. (a) Amplitude of specimen; (b) phase of specimen; (c) amplitude of probe light; (d) phase of probe light
    Error curves corresponding to the two calculation methods
    Fig. 7. Error curves corresponding to the two calculation methods
    Reconstructed results at the angle errors from -1.5° to 1.5°. (a) Reconstructed amplitude of probe light; (b) spectrum intensity of probe light; (c) amplitude of specimen; (d)error curve with the change of different angle errors
    Fig. 8. Reconstructed results at the angle errors from -1.5° to 1.5°. (a) Reconstructed amplitude of probe light; (b) spectrum intensity of probe light; (c) amplitude of specimen; (d)error curve with the change of different angle errors
    Part of diffraction patterns recorded by CCD, in which the coordinates represent the position information among the grid of 10×10
    Fig. 9. Part of diffraction patterns recorded by CCD, in which the coordinates represent the position information among the grid of 10×10
    Experimental results based on revised angular spectrum and ePIE with highly tilted illumination. (a) Amplitude of specimen; (b) phase of specimen; (c) amplitude of probe light; (d) phase of probe light
    Fig. 10. Experimental results based on revised angular spectrum and ePIE with highly tilted illumination. (a) Amplitude of specimen; (b) phase of specimen; (c) amplitude of probe light; (d) phase of probe light
    Experimental results based on general ePIE algorithm with highly tilted illumination. (a) Amplitude of specimen; (b) phase of specimen; (c) amplitude of probe light; (d) phase of probe light
    Fig. 11. Experimental results based on general ePIE algorithm with highly tilted illumination. (a) Amplitude of specimen; (b) phase of specimen; (c) amplitude of probe light; (d) phase of probe light
    Experimental error curves corresponding to the two calculation methods
    Fig. 12. Experimental error curves corresponding to the two calculation methods
    Experimental results of USAF 1951 test target. (a) Reconstructed results with the proposed algorithm; (b) locally enlarged view of Fig. 13 (a); (c) reconstructed results with the traditional ePIE algorithm; (d) locally enlarged view of Fig. 13 (c)
    Fig. 13. Experimental results of USAF 1951 test target. (a) Reconstructed results with the proposed algorithm; (b) locally enlarged view of Fig. 13 (a); (c) reconstructed results with the traditional ePIE algorithm; (d) locally enlarged view of Fig. 13 (c)
    Chengcheng Chang, Xingchen Pan, Hua Tao, Cheng Liu, Jianqiang Zhu. Reconstruction Algorithm for Ptychographic Iterative Engine with Highly Tilted Illumination[J]. Acta Optica Sinica, 2020, 40(17): 1705001
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