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Transcript of 11/8/99 SFR Workshop - Lithography 1 Small Feature Reproducibility A Focus on Photolithography...
11/8/99 SFR Workshop - Lithography
1
Small Feature Reproducibility
A Focus on Photolithography
UC-SMART Major Program Award
Spanos, Bokor, Neureuther
Second Annual Workshop
11/8/99
11/8/99 SFR Workshop - Lithography
2
Agenda
8:30 – 9:00 Introductions, Overview / Spanos
9:00 – 10:15 Lithography / Spanos, Neureuther, Bokor
10:15 – 10:45 Break
10:45 – 12:00 Sensor Integration / Poolla, Smith, Solgaard, Dunn
12:00 – 1:00 lunch, poster session begins
1:00 – 2:15 Plasma, TED / Graves, Lieberman, Cheung, Aydil, Haller
2:15 – 2:45 CMP / Dornfeld
2:45 – 3:30 Education / Graves, King, Spanos
3:30 – 3:45 Break
3:45 – 5:30 Steering Committee Meeting in room 775A / Lozes
5:30 – 7:30 Reception, Dinner / Heynes rm, Men’s Faculty Club
11/8/99 SFR Workshop - Lithography
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Litho Milestones, Year 1 Demonstrate AFM aerial image inspection on 180nm features. Demonstrate Specular Spectroscopic Scatterometry CD
metrology for 180nm features. Demonstrate focus classification scheme for 180nm features. Complete 3D device simulations of mask errors and LER
effects in gate-level. Threshold voltage shifts, turn-off characteristics, and saturated drain current will be evaluated.
Complete a simulation feasibility study and verification experiment on novel in-lens filtering for resolution enhancement.
Evaluate the physical basis for novel effects in interaction of light with materials and low voltage electrons with resists.
Establish web based simulation capabilities for DUV resists, mask topography effects and electron-beam lithography.
11/8/99 SFR Workshop - Lithography
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Litho Milestones, Year 2 Demonstrate AFM aerial image inspection on 50nm features. Demonstrate 150nm Specular Spectroscopic Scatterometry CD
metrology. Demonstrate focus classification scheme for 150nm features. Test NMOS devices with programmed mask errors and LER,
compare measured characteristics to simulation. Integrate scattering, imaging, resist modeling for analyzing
inspection and printabilty of mask non-idealities in the context of use with OPC.
Establish a prototype system for process integration including the automatic generation of simulation-designed multi-step, short loop test structures.
Establish web based simulation capabilities for optical alignment and advanced electron-beam lithography.
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Outline
• Simulation and Metrology– Lithography Simulator Calibration
– Scatterometry
– Plans for Statistical Process Optimization
• Line Edge Roughness• Lithography Simulation
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Thin film Spin Coat&
Soft Bake
Exposure&
PEBDevelop
Thicknessn and k
Thicknessn and k
Thicknessn and k
CD, profile andThickness
In-situ / On-wafer thin film Metrology– Reflectometry / Ellipsometry / Scatterometry
– Thickness, n & k, chemical composition
– Run-to-run and real-time monitoring
– Resist surface analysis for aerial image evaluation
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Motivation for Parameter Extraction
• Current lithography simulators are parameter limited as opposed to model limited.
• Traditional optimization techniques are unsuitable in complex, non-linear, high dimensional problems.
• Importance of predictive capabilities is increasing with increasing development costs and time-to-market pressures.
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Some Critical Parameters in DUV Lithography Simulation
Amplification Rate (Pre-exp)Amplification Rate (Activation)Acid Loss Rate (Pre-exp)Acid Loss Rate (Activation)Dill’s A ParameterDill’s B ParameterDill’s C ParameterRelative Quencher Conc.PEB Diffusivity (Pre-exp)PEB Diffusivity (Activation)
Maximum Develop RateMinimum Develop RateDeveloper SelectivityDeveloper Threshold PACResist Refractive Index (Real)Resist Refractive Index (Imag.)ARC Refractive Index (Real)ARC Refractive Index (Imag.)Relative FocusAmplification Reaction Order
•Exact values obtained from experiments or resist vendor•Narrow range of values available from unpatterned experiments•Wide parameter range
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Proposed DUV-SCAPE Framework
3: user specifiedparameter ranges
4: parameter interfacefront end
5: commercial simulation program
6: simulated profile
7: global optimizationengine (SAC)
2: image processingfront end
3: experimentalprofile
1: patterned resist experiments
1: unpatterned resist experiments
2: global optimizationengine (SAC)
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Salient Features
• Unpatterned Resist Models– BCAM exposure and bake models
– Mack develop model
• Optimization Technique– Global optimization theory (Adaptive Simulated Annealing)
• Patterned Resist Model– Existing lithography simulators (e.g. SAMPLE, Prolith,
Solid-C, etc.)
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Experiments - Commercial DUV Resist
• Unpatterned Resist Characterization Experiments– Process 4 wafers with flood exposed sites
– Measure ARC and Resist optical constants - Ellipsometry
– Measure exposure and PEB parameters - FTIR/DITL
– Measure develop parameters - DRM
• Patterned Resist Characterization Experiments– Process 1 wafer with a focus-exposure matrix
– Measure profiles for sub-quarter micron lines using AFM/cross-section CD-SEM/Specular Spectroscopic Scatterometry
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Unpatterned ExperimentsD
epro
tect
ion 140C 135C
120C
110C
Exposure Dose (mJ/cm2)
Dev
elop
Rat
e in
A/s
ec
3000
2000
1000
0 0 0.5 1Normalized concentration of unreacted sites
Exposure+ PEB
Parameters
DevelopParameters
0 1 2 3 4 5 6 7
1
.5
0
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Patterned Experiments: AFM vs Simulation
mask 1
mask 2
mask 3
mask 4
mask 5
-1 Focus +1 -1 Focus +1
Masks 1-10 differ in the line-space ratios
0.25 micron process technology
OPC assisted masks
mask 6
mask 7
mask 8
mask 9
mask 10
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What is Scatterometry?
• Concept: Scattering (Diffraction) of light from features produces strong structure in reflected optical field.
• Analyze structure to obtain topography information.
• Periodic structures (gratings) can be numerically modeled “exactly”.
Incident LaserBeam
0th order
Incident PolarizedWhite Light
0th order
2- Scatterometry Specular Spectroscopic Scatterometry
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Specular Spectroscopic Scatterometry0th order, broadband detection
1D gratings and 2D symmetric gratings
Use spectroscopic ellipsometersi 0
+1
-1
D
Cut-Off Pitch600 300400 200250 125 (in nm)
sinm = sini+m/D|sinm|<1
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TimbreProfilerTM
LibraryGeneration
TimbreProfilerTM
Measurement
Timbre ProfilerTM Flow
Generate Profile Library
Generate Signal Library
Timbre ProfilerTM
ElectromagneticSimulationSoftware
Load Libraryon Ellipsometer
Ellipsometer / Reflectometer
Compiled Profiler Library
Test Grating (Scribe Lane)
CollectReflected Signal
Ellipsometry Measurement
Reconstructed ProfileTotal Measurement + Analysis = 5 seconds/site
Analysis
Compiled Profiler Library
Typical turnaround time = 6-12 hours
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ProfilerTM Setup• Periodic grating on mask (~ 50 m * 50 m area - typical spot
size of production spectroscopic ellipsometers)– line/space specified
• Provide optical constants for each film in the stack– Broadband (240-800 nm)
• Specify variability expected in process (in CD & thickness)– range around nominal in nm
• Specify spectroscopic ellipsometer / reflectometer angle of incidence
• Save broadband tan and cos values
• Specify accuracy requirements– down to sub-nm (this automatically decides library size)
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GTK Interface at http://sfr.berkeley.edu
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Matching on tan() and cos()
Simulatedby GTK
Tan(
Cos(
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Example of 0.25m Profile Extraction
Blue isactual (by Veeco AFM).Red isextracted from GTK Library.
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Case I: Resist on ARC on Si (0.18 m technology)
Resist
ARC
Si
Focus-Exposure Matrix
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Profile Extraction over the entire FEM
RED isAFM.
BLUE isextracted.
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Offset between CD-SEM and ProfilerTM as a function of Sidewall Angle
bo
ttom
CD
(C
DS
EM
- P
XM
) in
nm
Sidewall angle in degrees
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Case II: Resist on ARC on Metal (0.m technology)
Focus-Exposure Matrix
Resist
ARC TiNAl
TiNTiTEOS
Si
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Profile Extraction: Resist on ARC on Metal
CD-SEM (Bottom CD)
PXM (Bottom CD)
Correlation* = 0.93
CD
(in
nm
)
Site Number
Profiler Extraction
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Case III: Etched Metal
Focus-Exposure Matrix
AlTiN
TiTEOS
Si
TiN
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Profile Extraction : Etched Metal
Profiler Extraction
CD-SEM (Top CD)
PXM (Top CD)
Site Number
CD
(in
nm
)
Correlation = 0.92
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But What Is Our Real Goal? -- a good profile ?
-- or high yield ?• We cannot avoid process variations
– Recipe setting drift: focus ( ~0.2 m), dose, PEB temperature
– Model and material parameter variation: resist n & k, developer Rmax and Rmin, acid diffusivity
– System inherent variation: mask OPC feature variation
• Our goal is to maximize yield for the statistical distribution of parameters and operating points.
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Parameter Variation Effect
Operating Point Settings
Pro
file
dev
iati
on f
rom
bes
t set
ting
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Parameter and Operating Point Variances Extraction
Experimentdata
Recipe setting+ drift
Parameter mean+ variation
Lithographyprocess
In-die spatialvariation
Hierarchical process disturbance extraction
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+-
RECIPEOPTIMIZER
Calibrated Lithography
Simulator
Simulated Output
distributions
Ope
rati
ng P
oint
dist
ribu
tion
s
Profileswithin spec.
Parameterdistributions
Spatialvariation
Overlapping to get yield
Recipe Optimization with Variations
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Recipe Optimization with Multiple Feature Types
Poly layerisolated lineperiodic lines with OPC
metal layerisolated lineperiodic lines with OPCelbowscombination of above
Need to link recipe optimization to circuit performance!
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Parameter relationship analysis
• In reality, all parameters have variations– too many dimensions for output distribution calculation
• Parameter relations can be analyzed to attribute the variation of some parameters to other parameters– diffusivity PEB temperature
– developer temperature Rmin and Rmax
• What are the fundamental reasons behind the variation?– Need a comprehensive list of disturbances, linked to physical
models, circuit performance.
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ExperimentData
Spatial variation filter
Param. & op.point variance
Param. mean values
Calibrated Sim. Eng.
Target Specs. of features
In-line sensor measurement
Recipe of max. yield
Maximization of overlapping area
Summary
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What is Next?
• Extend statistical optimization to other process steps– Plasma etching
– Metallization
– Device level
– Circuit level
• Process simulator for other steps needed– Simulator for full process procedure: Avant!, Solid C
– device model: BSIM3
– Circuit simulator: SPICE
• Study error budgets, linked to circuit performance.
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Outline
• Simulation and Metrology• Line Edge Roughness• Lithography Simulation
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Defining LER and Defect Specifications
SFR Workshop
November 08, 1999
Tho Nguyen, Shiying Xiong and J. Bokor
Berkeley, CA
The objective of this work is to understand and model the impact of lithography/etch line-edge roughness in the gate definition layer, on the electrical behavior of short channel
transistors
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Progress Since May
• Hydrodynamic Model working
• 3D interaction of Defects
• Real LER Simulation
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gate
n+ n+Cross-section
Layout views
Edge roughness
Single defects
Effect of Gate “Errors” on Device Characteristics
W
L
Threshold voltageTurn-off slopeDrive currentDevice reliability
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Base Design Channel Doping Selected at 0.4 Volt Halo Implant Incorporated to Offset Vt rolloff Threshold Swing 70-80 mV/decade @ Vds = 2V and L = 100nm DIBL = 70 mV/V for Vds = 0.05-2V
250
300
350
400
450
500
0 0.2 0.4 0.6 0.8 1 1.2
Vt RollOff Characteristics
Without Halo ImplantWith Halo Implant
Channel Length (Microns)
Device Length = 200 nmChannel Length = 100 nmChannel Width = 50-200 nmBuried Oxide = 100 nmSi Film Thickness = 250ÅGate Oxide = 30 Å
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160
Real 3D LER Construction and Simulation
• Real 3D LER Created by Matlab and incorporated into simulator language
• LER defined by band-limited white spectrum. 2 parameters: RMS roughness, correlation length
• Process simulation used for self-aligned S/D doping
• Current digitized LER resolution is 0.5-1nm due to limited memory
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Simulation Results• Hydrodynamic model has been
successfully turned on in ISE simulator
• With hydro on, Ion is ~ 30% higher• Simulations of “real” 3D LER has
been successful ( @ W = 50nm) Zoom View of Leakage Current
I_V Curves for Different Real 3D LER
25 % increase in Ioff for 5nm rms roughness
140% increase in Ioff for 9nm rms roughness
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Simulation Results• Defect shows 3D interaction for channel width
less than 100nm• To study LER, we have to use 3D models • Intel Work (T. Linton, et al. 1999):
• Simulation of square-wave modulation of LER with Neuman boundary conditions
• Shows similar 3D interaction
• Leakage control by length adjustment with reasonable Ion reduction 2 10-9
3 10-9
4 10-9
5 10-9
6 10-9
7 10-9
60 80 100 120 140 160 180 200 220
Ioff Varies With Channel Width
Ioff (No Defect)
Ioff(20nx20n Defect)
Channel With (nm)
0.00066
0.00068
0.0007
0.00072
0.00074
0.00076
60 80 100 120 140 160 180 200 220
Ion Varies with Channel Width
Ion (No Defect) [A/um]Ion(20nx20n Defect)
Channel With (nm)
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Milestone Status
• June 1999
– Complete 3D device simulations of mask errors and LER effects in
gate-level. Threshold voltage shifts, turn-off characteristics, and
saturated drain current will be evaluated.
– Status: Late. Student (Tho Nguyen) started Jan. 1999. Second student
(Shiying Xiong) started Sept. 1999. Expect completion March 2000.
• June 2000
– Test NMOS devices with programmed mask errors as well as varied
LER and compare measured characteristics with simulation results.
– Status: Delayed. No company fab support. Will start Microlab run
Jan. 2000 if unable to arrange support from company fab.
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Proposal for 2000-2002
Simulation• Effect of LER on GIDL• Effect of LER in isolation edge• Device reliability• Extend to 50 nm CD
Experiments• Complete gate roughness experiment for 100 nm CD• Isolation roughness experiment• Extend to 50 nm CD??
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Outline
• Simulation and Metrology• Line Edge Roughness• Lithography Simulation
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Implications of Polarization, Corner Rounding, OPC Design and OPC
Fidelity on Aerial Images
Konstantinos Adam
Prof. Andrew Neureuther UC Berkeley
• Use EM theory and rigorous TEMPEST simulations to investigate photomask technology issues• Current Investigations
• scattering bars - polarization effects• corners - interior versus exterior • OPC features - placement and corner rounding
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Scattering Bar Simulation with TEMPEST
m
mm
m
TE : Ey polarization
TM : Ex polarization
CDSB
x-axis
z-ax
is
Incident radiation
y-axis
CDtarget=130nmMag=4X=193nm
|Ey|
|Ex|
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SB Aerial Images
(m)
Nor
mal
ized
Int
ensi
ty=193nm, NA=0.7, =0.6, Mag=4X, CDtarget=130nm
Aerial Image (Best focus)
- Observe that the scatter bars (also the main feature) appear wider in TM excitation than in TE and narrower with SPLAT simulation (scalar theory)
0 0.1 0.2 0.3 0.4 0.50
0.2
0.4
0.6
0.8
1
1.2
1.4 SPLATTETM
No SB
SB size = 0.18/NA
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SB Design Graphs
Size of SB (/NA)C
D (
nm)
Size of SB (/NA)
Inte
nsit
y
0 0.05 0.1 0.15 0.2 0.25 0.3 0.350
.2
.4
.6
.8
1SPLATTETM
Perturbation model
Intensity dip of SB
0 0.1 0.2 0.3110
120
130
140
150
160 SPLATTETM
CD Control with SB Size Control
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Square
m
m m
m
Rounded
Corner Rounding (Clear Field Mask) - |Ey| Near fields
x-axis
y-ax
is
Ein
cide
nt (
TE
)
Ein
cide
nt (
TE
)
CDtarget=130nm
Mag=4X
=193nm
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Corner Rounding Design Graph
0 0.04 0.08 0.12 0.16 0.20
2
4
6
8
10
radius of curvature in /NA
LE
S in
cre
ase
fro
m r
efe
ren
ce in
nm
Clear field mask
Dark field mask
- LES increase versus radius of curvature is quadratic, i.e. it is proportional to the area missing from the corner due to the roundness
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External OPC – |Ey| Near Fieldsm
m m
m mm
Reference Square OPC “Mouse Ear” OPC
Example: 0.1/NA Square OPC and “Mouse Ear” OPC with radius=0.06/NA
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OPC Design Graph
0 0.2 0.4 0.6 0.8 1 1.2 1.4 1.6 1.8 20
5
10
15
20
25
non-overlapping area in m2 (1X)
LE
S c
orr
ectio
n in
nm
x10-3
Square OPC
“Mouse ear” OPC
Data for OPC displaced along the diagonal
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Resist modeling, Simulation and Line-End Shortening effects
Mosong Cheng
Prof. Andrew Neureuther, UC Berkeley
Use experiment and simulation to investigate photoresist performance and provide mechanism based models, characterization methodology, accurate profile simulation and support models/fast algorithms for including resist in OPC
Current investigations•chemically amplified resist modeling - LES and SFR K2G•electric-field-enhanced post-exposure bake •fast imaging algorithm for 2-dimensional OPC
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Resist-model-based line-end shortening simulation• APEX-E , UVIIHS, K2G parameter-extraction methodology
• Simulation flow
Problem: Top to Top underestimates diffusionProblem: Micro-stepper at Berkeley has insufficient image quality
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K2G resist: DRM curves and reaction/diffusion/outgasing model
• DRM curves, dissolution rate is lower at the top if no TARC.
• Reaction/diffusion/outgasing model
(x)CK- ).(
)1(
asC0
ae2
1
eDD
CKCDt
C
CCKt
C
aaa
maas
as
Collaborationwith Jacek TyminskiNikon
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K2G resist: modeling and simulation• Modeling methodology
Large-area exposure
Extracting
reaction rate
Extracting dissolution parameters
Fitting with DRM data
Extracting diffusivity
Resist profile simulation
• Fitting DRM curvesK2G without TARC
0
2
4
6
8
10
12
14
16
18
0 200 400 600 800z-Position [ nm ]
Dev
elop
men
t Rat
e [ n
m/s
ec ]
Simulation fordose6.7mJ/cm^2
DRM curvefor dose6.7mJ/cm^2
• Resist profile simulation
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Electric-field-enhanced post-exposure bake
• Goal: shorten PEB time, improve vertical resist profile uniformity, reduce lateral acid diffusion.
• Principle: vertical electric field enhance the vertical movement of photo-acid, hence enhance the reaction cross-section. PEB time as well as lateral acid diffusion can be reduced.
• Experimental Setup
Hotplate
Al foilwafer
Al foil
Resist Ephotoacid
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Electric-field-enhanced post-exposure bake: status
• Experiment done in summer 1999, on UVII resist using JEOL.
• UVII resist, 0.5µm L/S, dose 20µC/cm2, PEB with 100kHz, 3.3V AC, 140oC, 60sec.
• UVII resist, 0.5µm L/S, dose 20µC/cm2, nominal PEB,140oC, 90sec.
RESIST RESIST
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Fast resist imaging algorithm for 2-dimensional OPC(submitted to SPIE’99)
),(),,( gft
ggf
t
f
• Assume 2-D reaction/diffusion. Let f(x,y,t)=Cas(x,y,t), g(x,y,t)=Ca(x,y,t).
• Time-advancing scheme
factor relaxation:,,2
2)),,(),,,((.,
2
2)),,(),,,((.
,
)0,,(),,(,)0,,(),,(
222222
212
212
11
221
221
dddccct
tddtyxgtyxfd
t
tcctyxgtyxfc
t
gd
t
fc
tdtdyxgtyxgtctcyxftyxf
• Iterative solve c2,d2, to minimize the error E. 221
221 )2()2( tddtccE
Contains Spatial Laplacianand Uses 3rd Order Splines
Based on NT Aliasing and NL Relaxation
Very Fast as only requiresrepeated multiplication with fixed coefficients
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Fast resist imaging algorithm: simulating flow and tuning parameters
• Simulating and tuning flow:
Mask pattern SPLAT
aerial image
Resist imaging
resist profile
SEM picture
DifferentialResist
parameter tuner
• Extract resist parameters by tuning the image to fit with SEM picture.
Method of FeasibleDirection
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63
Progress on Milestones
• Year 1– simulate in-lens filtering (Done)
– resist exposure mechanisms (Not Started =>DARPA/SRC)
– web simulation resist and mask effects (In Progress 70%)
• Year 2– Integrate scattering, imaging and resist (Expanded by 3X in
the number of effects characterized, In Progress 70%)
– process flow generator for test structures (Not Started)
– web alignment and e-beam (alignment Ongoing 30%, e-beam Not Started => DARPA/SRC)
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Future Opportunities in Lithography
• Photomask EM effects (How to move faster?)– impact of non-idealities
– inspection and repair
• Chemically-Amplified Resists– models that work
– methodology to calibrate models for production
• Optical Systems– high NA
– low k1
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Targeted Opportunities in Photomasks and Optics
• Attenuating phase-shifting masks– high refractive index and physical height of the attenuating
material adversely influences light in adjacent areas
• Alternating phase-shifting masks– 3D problematical structures - resonate ridges and cross-talk
between features inside the photomask
• Phase-shifting mask repair– guidelines for adequate repair - height, slope, river bed,
stain• Optics
– role of laser bandwidth in image quality– high NA thin-film polarization effects
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Targeted Opportunities in Resists and Tools
• Complete comparison of Simulation and SEM's of printed features in K2G resist, quantify the accuracy of the resist model.
• Complete coding of the fast but approximate image processing like algorithm and assess speed and accuracy against rigorous simulation in STORM.
• Initiate tool-process-dependent line-end shortening investigation by identifying key factors contributing to line-end shortening and suggesting approaches for control and compensation tuning.