Chinese Journal of Lasers, Volume. 48, Issue 20, 2005001(2021)

Correction Technology for Illumination Field Intensity Profile in Photolithography Machine

Xiaozhe Ma1,2, Fang Zhang1、*, and Huijie Huang1,2、**
Author Affiliations
  • 1Laboratory of Information Optics and Optoelectronic Technology, Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Shanghai 201800, China
  • 2Center of Materials Science and Optoelectronics Engineering, University of Chinese Academy of Sciences, Beijing 100049, China
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    Figures & Tables(18)
    Optical system structure of step-and-scan lithography[11-16]
    Spatial distribution of top-Gaussian illumination field
    Generation principle of top-Gaussian illumination field
    In traditional illumination mode, the spot intensity distribution formed by a field point of view of the illumination light field on the light field correction plate. (a) Size of defocusing spot formation on the field correction plate; (b) intensity distribution of the defocusing spot on the field correction plate
    Simulation model of optical system for generating the top-Gaussian illumination field
    Illumination light field of three traditional lighting modes. (a) Illumination field 1; (b) illumination field 2; (c) illumination field 3
    Flow chart of transmittance distribution optimization algorithm of light field correction plate based on simulated annealing
    Tendency of Elost for three illumination fields during optimization. (a) Illumination field 1; (b) illumination field 2; (c) illumination field 3
    Transmittance distributions of three optimized correctors. (a) Corrector 1; (b) corrector 2; (c) corrector 3
    Comparison of the three illumination field intensity in non-scan and scan directions before and after correction. (a) Illumination field 1; (b) illumination field 2; (c) illumination field 3
    Simulation results of three corrected illumination fields. (a) Illumination field 1; (b) illumination field 2; (c) illumination field 3
    • Table 1. Requirements of the top-Gaussian illumination field

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      Table 1. Requirements of the top-Gaussian illumination field

      Non-scan directionScan direction
      DX/mmDuni/%DY_97 /mmDY_50 /mmDY_003 /mmDY_25~75 /mm
      ≥104≤0.304.2±0.513.2±0.422±1.5>2.9
    • Table 2. Design results of the microlenses of MLAs and diffuser

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      Table 2. Design results of the microlenses of MLAs and diffuser

      ElementSurface No.Surface typeRadius /mmConicThickness /mmMaterialComment
      MLAs1st MLA1Sphere1.602.00Fused silicaY MLA
      2Sphere-2.25X MLA
      2nd MLA3Aspheric0.50-0.390.75Fused silicaX MLA
      4Sphere-1.48Y MLA
      Diffuser1Sphereinf2.00Fused silica
      2Aspheric-0.70-2.78Y MLA
    • Table 3. Pitch distributions of the microlenses of MLAs and diffuser

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      Table 3. Pitch distributions of the microlenses of MLAs and diffuser

      No.Microlens’ pitch in non-scan direction /mmMicrolens’ pitch in scan direction /mm
      MLAs 10.520.19
      MLAs 20.520.19140.19150.19160.19170.1918
      0.19260.19340.19410.19490.1957
      MLAs 30.520.19590.19650.19680.19710.1975
      0.19820.19900.19980.20060.2014
      Diffuser0.00900.01900.02550.03200.0370
      0.04370.05000.05750.06780.8195
    • Table 4. Parameters of illumination light field of three traditional lighting modes

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      Table 4. Parameters of illumination light field of three traditional lighting modes

      No.Non-scan directionScan direction
      DX /mmDuni /%DY_97 /mmDY_50 /mmDY_003 /mmDY_25~75 /mm
      Illumination field 1107.601.443.7913.1827.863.69
      Illumination field 2107.551.444.1413.6827.963.69
      Illumination field 3107.551.444.3914.0827.963.72
    • Table 5. Parameters and energy loss of the three corrected illumination fields (correction results in non-scan direction)

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      Table 5. Parameters and energy loss of the three corrected illumination fields (correction results in non-scan direction)

      No.Elost /%Non-scan directionScan directionTime-consuming of optimization /s
      DX /mmDuni /%DY_97 /mmDY_50 /mmDY_003 /mmDY_25~75 /mm
      Illumination field 11.87104.060.243.7913.1827.863.647.68
      Illumination field 21.92104.010.154.1413.6827.963.647.34
      Illumination field 31.88104.060.174.3914.0827.963.677.61
    • Table 6. Parameters and energy loss of the three corrected illumination fields (final corrected results)

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      Table 6. Parameters and energy loss of the three corrected illumination fields (final corrected results)

      No.Elost /%Non-scan directionScan directionTotal time-consuming of optimization /s
      DX /mmDuni /%DY_97 /mmDY_50 /mmDY_003 /mmDY_25~75 /mm
      Illumination field 14.88104.060.263.7913.1823.463.379.15
      Illumination field 26.45104.010.194.1413.4823.463.158.87
      Illumination field 37.78104.060.224.3913.5823.463.009.09
    • Table 7. Parameters and energy loss of the three corrected lighting fields (simulation results)

      View table

      Table 7. Parameters and energy loss of the three corrected lighting fields (simulation results)

      No.Elost /%Non-scan directionScan directionTime-consuming of simulation /h
      DX /mmDuni /%DY_97 /mmDY_50 /mmDY_003 /mmDY_25~75 /mm
      Illumination field 14.76104.060.293.7913.1823.363.444
      Illumination field 26.34104.010.224.1413.4823.363.244
      Illumination field 37.67104.060.254.3913.5823.363.054
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    Xiaozhe Ma, Fang Zhang, Huijie Huang. Correction Technology for Illumination Field Intensity Profile in Photolithography Machine[J]. Chinese Journal of Lasers, 2021, 48(20): 2005001

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    Paper Information

    Category: Beam transmission and control

    Received: Feb. 8, 2021

    Accepted: Mar. 18, 2021

    Published Online: Sep. 22, 2021

    The Author Email: Zhang Fang (zhangfang@siom.ac.cn), Huang Huijie (huanghuijie@siom.ac.cn)

    DOI:10.3788/CJL202148.2005001

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