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Lecture 4: Lithography 2
Prasanna S. GandhiAssistant Professor,Department of Mechanical Engineering,Indian Institute of Technology, Bombay,
MEMS: Fabrication
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Recap: Last Class
LithographyOptical lithography
Contact printing Proximity printingProjection printing
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Today’s Class
E-beam lithographyX-ray lithographyIon beam lithographyOxidationSilicon wafer preparation processClean room fundamentals
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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 <1 micron ~ 20nm) features can be produced easily no diffraction limit: limitation due to electron scatterNot suitable for higher length featuresDeveloped in 1960s: SEM technology
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E-Beam Lithography
Mask making for optical lithographyDirect writing of ICsOpto-electronic devices, Quantum structures, Research applications:
Enhancement of contactCNT probe growth using Ebeam
Applications
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System DescriptionAn electron gun or electron source that supplies the electrons; An electron column that 'shapes' and focuses the electron beam; A mechanical stage that positions the wafer under the electron beam; A wafer handling system that automatically feeds wafers to the system and unloads them after processing; and A computer system that controls the equipment.
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Electron Gun
http://www.elettra.trieste.it/experiments/beamlines/lilit/htdocs/people/luca/tesihtml/node41.html
Cathode: Thermionicemmitter: tungstonhairpin, LaB6 OR field emmiters:
sintered material or crystal
Schottky emmitters
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Electronic GunM/c Electron Source
© FEI Beam Technology 2004
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E-Beam LithographyElectron Sources
100 hrs1000 hrs>1 year>1 yearTypical ServiceLife (hrs)
<1<14 - 6 <1Short-Term Beam Current Stability (%RMS)
1061071095 x 108Brightness (A/cm2SR
1.01.00.2 - 0.30.3 - 1.0Energy Spread (eV)
>104104315Source Size (nm)
TUNGSTENLaB6COLD FIELD
SCHOTTKY
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E-Beam Lithography
Schottky emmittersFor SEM of special resolution
Optics*
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E-Beam Lithography
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 , Raith, machineVariable beam shape m/c available
M/c: scanning
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E-Beam Lithography
Both positive and negative PRsExposure 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 resists
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Table: Negative and Positive ResisitsLithography Name Type Sensitivity γOptical Kodak 747 Negative 9 mJ/cm2 1.9
AZ-1350J Positive 90 mJ/cm2 1 .4PR102 Positive 140 mJ/cm2 1.9
e-beam COP Negative 0.3 µC/cm2 0.45GeSe Negative 80 µC/cm2 3.5PBS Positive 1 µC/cm2 0.35PMMA Positive 50 µC/cm2 1.0
X-ray COP Negative 175 mJ/cm2 0.45DCOPA Negative 10 mJ/cm2 0.65PBS Positive 95 mJ/cm2 0.5PMMA Positive 1000 mJ/cm2 1.0
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E-Beam Lithography
Line doseFor small scale fine featuresSpacing 100 ALow energy dose ~ 1.5nC/cm2
Area dose For bigger featuresSpacing 100 AHigh energy dose ~ 250 µC/cm2
Dose for PMMA
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SEM Images
Circular Gratings Rose
MEMS Device Radial Dots
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SEM Images
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Concept of Gray Exposure
Structure with varying dose More intensity/dose in areas requiring anchorsLess in areas requiring release
Structures that can be formedFilters, microchannels, polymer accelerometers, mechanisms
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Mechanical logic gate formed by Gray Exposure
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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
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Ion-beam Lithography
Better than electron beam in terms of resolution low scatter of ionsResists PMMAPerceived as a ‘next generation’ lithography process
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Oxidation
Oxidation of Si*: keep in air at high temp (1000-1200oC)Well understood and controlled processDry and wet oxidation
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Oxidation
ParametersTemperatureEnvironmentTime
Oxide uses from MEMS perspectiveSacrificial layer Important patterning material
Problems: thermal stresses
Bdt
dTAT
BAtBATT
oxox
oxox
=+
+=+
2
Constants,)(2 τ
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Oxidation
ParametersTemperatureEnvironmentTime
At smaller thicknessAt higher thicknessInitial time τ corresponds to initial oxide thickness
2 ( ), Constants
(2 )
ox ox
oxox
T AT B tA B
dTT A Bdt
τ+ = +
+ =
)(/ τ+= tABTox
)( τ+= tBTox
0
10
20
2
2
DN
Nk
Ddds
+
=τ
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Oxidation
Parameters
0
10
20
2
2
DN
Nk
Ddds
+
=τ
016 2 0
016
initial oxide layer (200A in dry oxdn, 0 for wet)
Diffusivity of oxide in Si e.g. D 4 4 10 / at 900Surface reaction rate constant Conc. of oxygen molecules in carrier gas
5.2X10
s
d
D . X cm s CkN
m
−
=
= ===
= 3 02
122 3
2 2
/ in dry O at 1000 and 1 atm No of oxidizing species in the oxide
2.2X10 SiO / in dry O
olecules cmN
molecules cm
=
=
25
Oxidation
Parameters
Knowing thickness by observing the color (rough estimate)
bTaB
bTaAB
+′=
+′=
)ln(
log
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Ruska 1987, Madou 1997, and van Zant 1997.
Table Color of silicon dioxide layers of selected thicknessSiO2LayerThicknes, 0.275 0.310µm 0.050 0.075 0.465 0.493 0.50 0.375 0.390
Color Tan Brown Red- Blue Green to Green- YellowViolet yellow- yellow
green
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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
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Next class
Si wafer preparationClean room fundamentalsChemical etching processAnisotropic Etching
The following class: Plasma processes