Chinese Journal of Lasers, Volume. 51, Issue 7, 0701006(2024)

Stochastics in EUV Lithography and Recent Research Status

Xiang Wang, Jianjun He, Jialiang Wei, and Huie Zhu*
Author Affiliations
  • Zhangjiang Laboratory, Shanghai 201210, China
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    Figures & Tables(16)
    Photoresist exposure process and origin of EUV stochastics in different lithography processes
    Differences between traditional and stochastic failures[5]. (a) Stochastic failures; (b) traditional types of defects
    Scheme showing the radiation chemistry mechanisms of EUV resists[14-15]
    Absorption cross sections of elements (Z=1‒86) at EUV[24]
    Line-edge roughness (LER) values after the entire CAR patterning process in low Tg and high Tg[85]. (a) LER as a function of the protected site ratio fp when the number of beads N=64; (b) LER as a function of the number of beads N at fixed fp=0.5; (c) 3D image of residual polymer from (a) for low Tg resist; (d) 3D image of residual polymer from (b) for low Tg resist
    Sequence controlled resists based on polypeptoid [86]. (a) Scheme showing monomer structures and polymer sequence; (b) patterns produced from polypeptoid of different sequences under DUV exposure
    Concept and lithographic results of novel functionalized materials[74]
    Defect analysis for BQ variation[75]. (a) Total post litho defect density with e-beam; (b) nanobridge defect density; (c) line break defect density
    Process flow of PTD (positive-tone development) and NTI (negative-tone imaging) lithography[89-90]
    Process windows for line/space between EUV PTD and EUV NTD[92]
    Distribution of light intensity on high reflective substrate and a baking step smoothens this concentration pattern by diffusion (from the left to the right shows the chronological sequence of a numerical modelling)[94]
    Simulation results of LCDU (3σ) variation of 20 nm half pitch (HP) dense hole pattern with cluster diameter (same imaging conditions)[95]
    Schematic of the fully coupled Monte Carlo simulation for calculating reaction distributions in resist films[120]
    Stochastic effect analysis based on Monte Carlo method[15,120]. (a) Monte Carlo simulated photon adsorption (red ball), secondary electron generation (blue ball), and acid-induced deprotection reaction (green dot) in DUV and EUV CAR; (b) probability model of the stochastic effect for statistical analysis
    Framework of the multiscale computation simulation model[124]. (a) Density functional theory (DFT), molecular dynamics (MD), and finite difference method (FDM) combined computational study of the exposure process of EUV photoresist materials; (b) simulating the effect of PEB time on exposed morphology
    • Table 1. Structure, density and linear absorption coefficient of selected polymers[23]

      View table

      Table 1. Structure, density and linear absorption coefficient of selected polymers[23]

      NameStructureFormula

      Density /

      (g·cm-3

      Calculated linear absorption

      coefficient /μm-1

      Measured linear absorption

      coefficient /μm-1

      PMMAC5H8O21.185.195.03
      PNBC7H100.922.552.58
      PStC8H81.052.952.70
      PHOStC8H8O1.164.053.88
      PTMSStC11H16Si1.142.782.14
      PMPSC7H8Si1.122.602.82
      PPSSQC24H20Si4O41.504.524.45
      PAFC15H14O3F121a6.9710.75
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    Xiang Wang, Jianjun He, Jialiang Wei, Huie Zhu. Stochastics in EUV Lithography and Recent Research Status[J]. Chinese Journal of Lasers, 2024, 51(7): 0701006

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    Paper Information

    Category: laser devices and laser physics

    Received: Dec. 11, 2023

    Accepted: Jan. 23, 2024

    Published Online: Apr. 17, 2024

    The Author Email: Huie Zhu (zhuhe@zjlab.ac.cn)

    DOI:10.3788/CJL231499

    CSTR:32183.14.CJL231499

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