Laser & Optoelectronics Progress, Volume. 59, Issue 9, 0922020(2022)

Key Technologies and Applications of Excimer Laser as Light Sources in Lithography

Rui Jiang1,2、*
Author Affiliations
  • 1Optoelectronic Technology R&D Department, Beijing Institute of Microelectronics, Chinese Academy of Sciences, Beijing 100029, China
  • 2Beijing RSLaser Opto-Electronics Technology Co., Ltd, Beijing 100176, China
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    Figures & Tables(27)
    Schematic diagram of potential energy for ArF excimer laser[1]
    Position of lithography system in integrated circuit technology and schematic diagram of lithography system. (a) Position; (b) schematic diagram
    Trend of exposure wavelength reduction and theoretical resolution limit for laser source of lithography system[1]
    Diagram of E95 and FWHM
    Schematic of single-chamber excimer laser system
    Cross section of discharge chamber[10]
    Schematic of dual-chamber excimer laser system
    Light path of MOPA dual-chamber
    Ring light path of MOPRA dual-chamber
    Light path of injection lock structure
    Schematic of clearance in discharge region[1]
    Basic schematic of gas lifetime controller system[40]
    Diagram of light propagation
    Intensity distributions of Gaussian mode and excimer mode and their curves of knife edge. (a) Beam of Gaussian fundamental mode[48]; (b) beam of excimer laser[48]; (c) relationship between knife edge ratio ∈ and Dc/σx for several Gaussian modes[49]
    Recent excimer laser source is improved in many aspects, including production ratio, durability and optical performance
    Concept schematic of Gigaphoton hTGM Neon recycling system[54]
    Concept schematic of Cymer XLGR Neon recycling system[56]
    Relationship between change of E95 and change of critical dimension is basically linear correlation
    Excimer laser inspection system ExciStar S-Industrial designed by Coherent Inc[64]
    Cross section of fiber structure used in laser inspection system[65]
    • Table 1. Wavelengths of different excimer lasers

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      Table 1. Wavelengths of different excimer lasers

      HalogenExcimer laser gasmixture
      ExcimerF2ArFKrClKrFXeBrXeCLXeF(B-X)
      Wavelength /nm157193222248262308351
    • Table 2. Development history of excimer lasers

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      Table 2. Development history of excimer lasers

      YearResearch institutionLandmark of progression
      1970Lebedev Physical Institute in MoscowThe first excimer lasing was invented
      1974University of Cambridge,Cambridge,UK;Kansas State University,Kansas,USA;Avco Everett Research Laboratory,Everett,Massachusetts,USAThe fluorescence spectra of rare-gas halides were investigated
      1975Naval Research Laboratory,Washington,USA;Northrop Research and Technology Center,Hawthorne,USA;Avco Everett Research Laboratory,Everett,Massachusetts,USA;Sandia Laboratories,Albuquerque,USAThe first laser of exciplexes was demonstrated
      1979Lambda PhysikThe first commercial excimer laser system was developed
      1980IBMJain proposed the concept of excimer laser on lithography
      1980IBMThe lithographic exposure experiment by excimer lasers in contact mode was carried out
      1982IBMWith the modified Micralign system,the projection lithography by excimer laser was experimentally demonstrated
    • Table 3. Some models of lithography systems for ASML, Nikon and Canon, and laser sources of these systems

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      Table 3. Some models of lithography systems for ASML, Nikon and Canon, and laser sources of these systems

      CompanyModelExposure typeResolution /nmLaser sourceNAOutput rate(Wafer /h)
      ASMLNXT1980DiDouble immersion step-and-scan exposure38193 nm ArF1.35275
      NXT1950i175
      XT1450HDouble dry step-and-scan exposure650.93162
      XT1000K80248 nm KrF180
      XT860K1100.80210
      XT400K350365 nm high pressure mercury lamp0.65220
      PAS5500/1150CSingle step-and-scan exposure90193 nm ArF0.75135
      PAS5500/850DNA110248 nm KrF0.80145
      PAS5500/450FNA220365 nm high pressure mercury lamp0.65150
      NikonNSR-S631Eimmersion step-and-scan exposure38193 nm ArF1.35270
      NSR-S621D200
      NSR-S322Fstep-and-scan exposure65248 nm KrF0.92230
      NSR-S210D1100.86176
      CanonFPA-6300ES6astep-and-scan exposure90248 nm KrF0.86200
    • Table 4. Influence of laser source parameters on critical dimension of lithography system

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      Table 4. Influence of laser source parameters on critical dimension of lithography system

      Critical dimension
      LithographyLens aberrationsFocusDose controlOptical proximity effectIllumination
      LasersLinewidthWavelength stabilityEnergy stabilityBandwidth stabilityBeam stability
      Spectral shapeBeam stabilityBeam stabilityDegree of polarization
    • Table 5. Relationship of process node with linewidth and center wavelength stability

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      Table 5. Relationship of process node with linewidth and center wavelength stability

      Process node /nmTypeLinewidth(FWHM)/pmCenter wavelength stability /pm
      180‒110KrF single-chamber≤0.35‒0.60≤0.050
      90‒65ArF dual-chamber,dry≤0.25≤0.030
      45‒28ArF dual-chamber,immersion≤0.25≤0.030
      14ArF dual-chamber,immersion,multiple exposure≤0.25≤0.018
      7ArF dual-chamber,immersion,multiple exposure≤0.25≤0.012
    • Table 6. Comparison of gas reduction and recycling between Cymer and Gigaphoton in recent years

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      Table 6. Comparison of gas reduction and recycling between Cymer and Gigaphoton in recent years

      YearCymerGigaphoton
      2015With GLX system and Neon reduction system,75% of Neon usage is saved for XLR700ixHelium is replaced by Nitrogen for GT64A,and it saves 80 kL Nitrogen per year;For GT63A,with help of eTGM Neon reduction system,usage of Neon is reduced from 200 kL per year to 100 kL per year
      2016
      2017
      2018On basis of Neon reduction system,90% Neon is saved by XLGR Neon recycling system for XLR800ixOn basis of eTGM,92% Neon is recycled by hTGM Neon recycling system for GT65A
      2019
    • Table 7. Comparison of laser lifetime between Cymer and Gigaphoton in recent years

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      Table 7. Comparison of laser lifetime between Cymer and Gigaphoton in recent years

      YearCymerGigaphoton
      2015Maximum lifetime of XLR700ix is 90 billion pulsesMaximum chamber lifetime of GT64A is 40 billion pulses
      2016
      2017
      2018Maximum chamber lifetime of XLR800ix is 120 billion pulsesMaximum chamber lifetime of GT64A is 60 billion pulses
      2019
      2020Expected maximum chamber lifetime of XLR900ix is 180 billion pulsesMaximum chamber lifetime of GT66A-1 is 100 billion pulses
      FutureNAMaximum chamber lifetime of GT66A-1 is 120 billion pulses and maximum line narrowing module lifetime is 180 billion pulses
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    Rui Jiang. Key Technologies and Applications of Excimer Laser as Light Sources in Lithography[J]. Laser & Optoelectronics Progress, 2022, 59(9): 0922020

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    Paper Information

    Category: Optical Design and Fabrication

    Received: Feb. 10, 2022

    Accepted: Apr. 10, 2022

    Published Online: May. 10, 2022

    The Author Email: Jiang Rui (jiangrui@ime.ac.cn)

    DOI:10.3788/LOP202259.0922020

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