Chinese Optics, Volume. 17, Issue 5, 1183(2024)

An MTF calculation model under the influence of ghost images

Peng-yi XIAO1,2, Ming-xin LIU1、*, Lei YAN1, Ming-yu HU1, and Xin ZHANG1
Author Affiliations
  • 1Changchun Institute of Optics, Fine Mechanics and Physics, Chinese Academy of Sciences, Changchun 130033, China
  • 2University of Chinese Academy of Sciences, Beijing 100049, China
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    Figures & Tables(12)
    Schematic diagram of ghost image path of a single lens
    MTF calculation flowchart
    MTF curves calculated by two methods under four types of ghost image paths
    MTF curves calculated by two methods under ghost image path 3_2
    Schematic diagram of illuminance distribution of ghost image beams on image plane under 3_2 path calculated by non-sequential ray tracing
    MTF curves calculated by two methods under 6_1 ghost image path
    Schematic diagram of illumination distribution of ghost image on image plane under 6_1 path calculated by non-sequential ray tracing
    • Table 1. Calculation expressions for E0, where the blue lines in the schematic diagram of the ghost image beam represent the ghost image rays and black ones represent the imaging rays

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      Table 1. Calculation expressions for E0, where the blue lines in the schematic diagram of the ghost image beam represent the ghost image rays and black ones represent the imaging rays

      序号鬼像光束示意图E0表达式
      1$ {E_0} = \dfrac{{{n_k}[{h_k}{u_{kg}} - {h_{kg}}{u_k}]}}{H} $
      2$ {E_0} = \dfrac{{{n_k}[{h_k}{u_{kg}} + {h_{kg}}{u_k}]}}{H} $
      3$ {E_0} = \dfrac{{{n_k}[{h_{kg}}{u_k} - {h_k}{u_{kg}}]}}{H} $
    • Table 2. Transmission matrices for all surfaces

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      Table 2. Transmission matrices for all surfaces

      透射矩阵反射矩阵
      前表面$ {{\boldsymbol{M}}_{{1}}}{{ = }}\left[ {\begin{array}{*{20}{c}} {{1}}&{{0}} \\ {{{ - }}\dfrac{{{{n' - 1}}}}{{{{n'}}{{{r}}_{{1}}}}}}&{\dfrac{{{1}}}{{{{n'}}}}} \end{array}} \right] $$ {{\boldsymbol{M}}_{{{11}}}}{{ = }}\left[ {\begin{array}{*{20}{c}} {{1}}&{{0}} \\ {{{ - }}\dfrac{{{2}}}{{{{{r}}_{{1}}}}}}&{{{ - 1}}} \end{array}} \right] $
      后表面$ {{\boldsymbol{M}}_{{2}}}{{ = }}\left[ {\begin{array}{*{20}{c}} {{1}}&{{0}} \\ {{{ - }}\dfrac{{{{1 - n'}}}}{{{{{r}}_{{2}}}}}}&{{{n'}}} \end{array}} \right] $$ {{\boldsymbol{M}}_{{{22}}}}{{ = }}\left[ {\begin{array}{*{20}{c}} {{1}}&{{0}} \\ {{{ - }}\dfrac{{{2}}}{{{{{r}}_{{2}}}}}}&{{{ - 1}}} \end{array}} \right] $
    • Table 3. Triplet lens parameter data (Unit: mm)

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      Table 3. Triplet lens parameter data (Unit: mm)

      表面曲率半径厚度材料
      13.2851N-LASF31A
      2−30.010.142
      3−6.7690.9SF15
      42.4890.673
      56.311N-LAK21
      6−4.88910.6713
    • Table 4. The stray light rates and MTF values under the influence of ghost image in all paths

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      Table 4. The stray light rates and MTF values under the influence of ghost image in all paths

      路径杂光率$ MTF' $$ MTF $之间的关系
      2_10.058858$ MTF'=0.944\;413MTF $
      3_20.877073$ MTF'=0.532\;744MTF $
      3_10.029316$ MTF'=0.971\;518MTF $
      4_30.008263$ MTF'=0.991\;804MTF $
      4_20.005352$ MTF'=0.994\;676MTF $
      4_10.061024$ MTF'=0.942\;485MTF $
      5_40.119049$ MTF'=0.893\;615MTF $
      5_30.006792$ MTF'=0.993\;252MTF $
      5_20.004984$ MTF'=0.995\;040MTF $
      5_10.019154$ MTF'=0.981\;20MTF $
      6_50.067233$ MTF'=0.937\;001MTF $
      6_40.064353$ MTF'=0.939\;534MTF $
      6_30.037417$ MTF'=0.963\;936MTF $
      6_20.018945$ MTF'=0.981\;406MTF $
      6_10.044890$ MT{F}'=0.957\;038MTF $
    • Table 5. MSE values under all ghost image paths

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      Table 5. MSE values under all ghost image paths

      路径MSE值
      2_11.253505×10−4
      3_21.826590×10−2
      3_13.627304×10−5
      4_32.866007×10−6
      4_22.798693×10−5
      4_17.217275×10−4
      5_41.933488×10−4
      5_31.222153×10−5
      5_29.061267×10−6
      5_15.363379×10−5
      6_54.459207×10−4
      6_41.627363×10−4
      6_34.774974×10−5
      6_21.692015×10−5
      6_14.937398×10−2
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    Peng-yi XIAO, Ming-xin LIU, Lei YAN, Ming-yu HU, Xin ZHANG. An MTF calculation model under the influence of ghost images[J]. Chinese Optics, 2024, 17(5): 1183

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    Paper Information

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    Received: Jul. 21, 2023

    Accepted: --

    Published Online: Dec. 31, 2024

    The Author Email:

    DOI:10.37188/CO.2023-0121

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