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MEMS: Fabrication Lecture 4: Lithography 2 Prasanna S. Gandhi Assistant Professor, Department of Mechanical Engineering, Indian Institute of Technology, Bombay,

Lecture 4: Lithography 2gandhi/me645/L4_Lithography2oxdn_etch.pdf · Lithography 2 Prasanna S. Gandhi Assistant Professor, Department of Mechanical Engineering, Indian Institute of

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  • MEMS: Fabrication

    Lecture 4: Lithography 2

    Prasanna S. GandhiAssistant Professor,Department of Mechanical Engineering,Indian Institute of Technology, Bombay,

  • Recap: Last Class

    LithographyOptical lithography

    Contact printing Proximity printingProjection printing

  • Today’s Class

    E-beam lithographyX-ray lithographyIon beam lithographyOxidationSilicon wafer preparation processClean room fundamentals

  • E-Beam Lithography

    Features are written by scanning 10-50keV electron beamNo necessity of maskCan be used for preparation of maskVery fine size (sub-micron or

  • E-Beam LithographyApplications

    Mask making for optical lithographyDirect writing of ICsResearch applications:

    Nano-manipulator / probe growth using CNTFine structures

  • E-Beam Lithography

    Cathode: Thermionicemmitter: tungstonhairpin, LaB6 OR field emmiters: sintered material or crystalSchottky emmitters

    M/c Electron Source

    © FEI Beam Technology 2004

  • E-Beam LithographyElectron Sources

    SCHOTTKY COLD FIELD

    LaB6 TUNGSTEN

    Source Size (nm)

    15 3 104 >104

    Energy Spread (eV)

    0.3 - 1.0 0.2 - 0.3 1.0 1.0

    Brightness (A/cm2SR

    5 x 108 109 107 106

    Short-Term Beam Current Stability (%RMS)

  • E-Beam LithographyOptics*

    Schottky emmittersFor SEM of special resolution

  • E-Beam LithographyM/c: scanning

    Scanning *Raster scanVector scanOnce i is set, exposure is controlled by varying speed v and scan spacing s

    Stepping:F = 0.25 to 6mmStage movement for scanning the next field

    JEOL EBL machineVariable beam shape m/c available

  • E-Beam LithographyE-beam resists

    Both positive and negativeExposure dose charge/cm2

    Parameter γ: slope of thickness vsexposure curve * Resolution depends on electron scatter, better for smaller thicknessPMMA + (γ=2), COP - (Mead Tech) (γ=0.8)

  • E-Beam LithographyDose for PMMA

    Line doseFor small scale fine featuresSpacing 100 ALow energy dose ~ 1.5nC/cm

    Area dose For bigger featuresSpacing 100 AHigh energy dose ~ 250 µC/cm2

  • X-ray Lithography

    High aspect ratio structuresOptical materials opaque to small wavelengths but transparent to x-raysAll electron resists are also x ray resist, because photoelectrons produced during x-ray absorptionPMMA resist is usually usedX-ray masks different from cr optical masks: e.g. Gold with thickness 0.7µm, 0.5µm, 0.2µm for l 4.4A (Pd), 8.3A (Al), 13.3A (Cu). Metal is thicker than crMask substrates?? Polyamide, SiC, Si3N4, Al2O3

  • Ion-beam Lithography

    Better than electron beam in terms of resolution low scatter of ionsResists PMMAPerceived as a ‘next generation’ lithography process

  • Oxidation

    Oxidation of Si*: keep in air at high temp (1000-1200oC)Well understood and controlled processDry and wet oxidation

  • Oxidation

    ParametersTemperatureEnvironmentTime

    Oxide uses from MEMS perspectiveSacrificial layer Important patterning material

    Problems: thermal stresses

    Bdt

    dTAT

    BAtBATT

    oxox

    oxox

    =+

    +=+

    2

    Constants,)(2 τ

  • Conclusions

    E-beam lithography: high precision applications, mask preparationX-Ray lithography: expensive and hazardous useful for high aspect ratioIonbeam lithography: Better resolution than e-beam possibleOxidation

  • Next class

    Si wafer preparationClean room fundamentalsChemical etching processAnisotropic Etching

    The following class: Plasma processes

    Lecture 4: Lithography 2