Coherence Scanning Mircroscope
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Transcript of Coherence Scanning Mircroscope
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2/27/2013
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SureshK.RamasamyPhDMarch 2013
COHERENCESCANNINGINTERFEROMETRY
Part1.Basics,CalibrationandAdjustment
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Noncontact areal surface measurement systems Coherence scanning interferometer Standards ISO, ASME Part standards Vibration test Calibration, adjustment procedures Objective focus optimization
Email id: [email protected]
OUTLINE
Sciencestartswheremeasurementstarts D.I.Mendeleev
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QUESTIONS?
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Potential3DMeasurementInstruments
Contacting StylusChromatic Length Aberration Confocal MicroscopySEM StereoscopyScanning Tunneling MicroscopyAtomic Force MicroscopyOptical Difference Profiling Angle Resolved SEM
Areal TopographySenses Z(X,Y) or
Z(X) as a function of Y
TriangulationFastMoirInterferometerConfocalMicroscopePhaseShiftingInterferometerVerticalScanning(WhiteLight)Interferometer
Promise Speed & accuracy Laboratory
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Triangulation
1 . F a n g J u n g S h i o u , M i n X i n L i u , D e v e l o pm e n t o f a n o v e l s c a t t e r e dt r i a n g u l a t i o n l a s e r p r o b e w i t h s i x l i n e a r c h a r g e c o u p l e d d e v i c e s ,O p t i c s a n d L a s e r s i n E n g i n e e r i n g , 4 7 ( 2 0 0 9 ) 7 1 8
2 . S t a g e o n e : L i g h t R e f l e c t i o n Mo d e l s f r om we b s i t eh t t p : / /www . g r a p h i c s . c o r n e l l . e d u / r e s e a r c h / g l o b i l l um / r e f l mo d e l . h tm l ,a s o f 0 5 / 0 5 / 2 0 1 0
Working principle of a triangulation probe based on Scheimpflugs principle
Bi-directional reflectance distribution model
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MoirInterferometer
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ChromaticLengthAberration
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Top
Bottom
ConfocalMicroscopy
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-20 -10 0 10 20z axis (micrometers)
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1.0
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Focu
s fu
nctio
n Intensity
Fig 3b20X
Gradient
LED Light source480 nm
PBS Microdisplay
CCD
Objective
ConfocalMicroscopy
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Waves of Light
Wavelength
Light is comprised of wavelengths of energy
The length determines the color of l ight
White l ight (a combination of different wavelengths) provides a larger measurement range.
TheoryofLight
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Interference is the phenomenon caused by superposition of two electromagnetic waves
When these two waves are in phase then the result is a bright band and if they are out of phase the result would be a dark band
Mathematical Representation :
is the interference term.
(2 1) is the phase difference between two waves.
Constructive Interference
Destructive Interference
TheoryofInterference
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TheoryofInterference
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SampleSurfacesandtheirpatterns
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WLI.Underthehood
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Differentwaystofindthepeak
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InterferenceFringes
Fromfringesto3Dsurfacemap
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CoherenceScanningInterferometera
b
d
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f
gh
ijl
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a Light source (halogen / LED)b Dichoric mirrorc Laser source (optional)d Opticse Aperture stopf Field stopg 45 Mirrorh Beam splitteri Interferometric objectivej Reference mirrork Measured surfacel Scanner (PZT / Stepper motor)m Zoom / magnification tube setupn Beam splittero Polarizer (Optional)p Detector 2 (Optional)q Polarizerr Detector 1 (CCD / CMOS)
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CoherenceScanningInterferometera
b
d
e
f
gh
ijl
n
m
r
q
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a Light source (halogen / LED)b Dichoric mirrorc Laser source (optional)d Opticse Aperture stopf Field stopg 45 Mirrorh Beam splitteri Interferometric objectivej Reference mirrork Measured surfacel Scanner (PZT / Stepper motor)m Zoom / magnification tube setupn Beam splittero Polarizer (Optional)p Detector 2 (Optional)q Polarizerr Detector 1 (CCD / CMOS)
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CoherenceScanningInterferometera
b
d
e
f
gh
ijl
n
m
r
q
k
a Light source (halogen / LED)b Dichoric mirrorc Laser source (optional)d Opticse Aperture stopf Field stopg 45 Mirrorh Beam splitteri Interferometric objectivej Reference mirrork Measured surfacel Scanner (PZT / Stepper motor)m Zoom / magnification tube setupn Beam splittero Polarizer (Optional)p Detector 2 (Optional)q Polarizerr Detector 1 (CCD / CMOS)
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CoherenceScanningInterferometera
b
d
e
f
gh
ijl
n
m
r
q
k
a Light source (halogen / LED)b Dichoric mirrorc Laser source (optional)d Opticse Aperture stopf Field stopg 45 Mirrorh Beam splitteri Interferometric objectivej Reference mirrork Measured surfacel Scanner (PZT / Stepper motor)m Zoom / magnification tube setupn Beam splittero Polarizer (Optional)p Detector 2 (Optional)q Polarizerr Detector 1 (CCD / CMOS)
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CoherenceScanningInterferometera
b
d
e
f
gh
ijl
n
m
r
q
k
a Light source (halogen / LED)b Dichoric mirrorc Laser source (optional)d Opticse Aperture stopf Field stopg 45 Mirrorh Beam splitteri Interferometric objectivej Reference mirrork Measured surfacel Scanner (PZT / Stepper motor)m Zoom / magnification tube setupn Beam splittero Polarizer (Optional)p Detector 2 (Optional)q Polarizerr Detector 1 (CCD / CMOS)
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CoherenceScanningInterferometera
b
d
e
f
gh
ijl
n
m
r
q
k
a Light source (halogen / LED)b Dichoric mirrorc Laser source (optional)d Opticse Aperture stopf Field stopg 45 Mirrorh Beam splitteri Interferometric objectivej Reference mirrork Measured surfacel Scanner (PZT / Stepper motor)m Zoom / magnification tube setupn Beam splittero Polarizer (Optional)p Detector 2 (Optional)q Polarizerr Detector 1 (CCD / CMOS)
c
p o
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NT8000 (Veeco) CCI (Taylor Hobson) NV6300 (Zygo)
ExamplesofCSIsystems
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Configurations
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ISOStandards ISO / TC 213 / WG16 25178
NominalCharacteristics 602 Confocalchromaticprobe 603 Phaseshifting interferometric microscopy 604 Coherencescanning interferometric microscopy 605 Pointautofocusprobe 606 Focusvariation 607 ImagingconfocalmicroscopyCalibration 702 Confocalchromaticprobe 703 Interferometric microscopy
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NPLGPGs Good Practice Guide No. 108: Guide to the Measurement of
Smooth Surface Topography using Coherence Scanning Interferometry
Good Practice Guide No. 116: Guide to the Measurement of Rough Surface Topography using Coherence Scanning Interferometry
Giusca CL, Leach RK, Calibration of the metrological characteristics of areal surface topography measuring instruments, Proceedings of the 2nd International Conference on Surface Metrology 2010, WPI, USA pp. 145153.
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ReferenceFlatStandard Silicon Carbide Surface SubAngstrom level flatness Used to establish bestcase measurement capability
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StepHeightStandard Chromium coated on etched Quartz surface NIST Traceable Calibration and adjustment of Z axis measurements
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LateralCalibrationStandard Platinum coating on etched Silicon dioxide surface NIST Traceable Setting magnification and TRC
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OpticalDimensionalStandard Chrome on glass photomask NPL Traceable
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SurfaceRoughnessSpecimens ISO 5436 1:2000
TypeC(Spacingmeasurementstandards) TypeD(Roughnessmeasurementstandards)
NIST Traceable ITF and Algorithm depenedencies
a
b
c
Cross sectional profiles of (a) random surface (b) sinusoidal surface and (c) square wave surface.
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Siemens Star
Weckenmannetal,Practiceorientedevaluationoflateralresolutionformicro andnanometermeasurementtechniques,MeasurementScienceandTechnology,20(2009)065103(8pp)
ITF and Algorithm dependencies
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Vibrations
(a) Measurements taken under ideal environment (b) under high vibration levels, seen as ripples of missing data.
a b
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Vibrations
y = 0.6255x + 2.3434R2 = 0.9951
0
50
100
150
200
250
300
0 100 200 300 400 500
Peak to peak noise level (nm)
Mea
suremen
t error
(1 S
igma in nm)
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Calibration
Z axis Systemswithreferencesignal Systemswithoutreferencesignal
Stepheightartifactbasedusercalibration XY axis
Presetmagnification Usertunablemagnification
Lateralcalibrationstandardbasedusercalibration Specificforeachobjectiveandzoomtubesetting Linear doesntincludewarpingerrors
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ZaxisCalibration
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LateralCalibration
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LateralCalibration steps
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TRCSetup
Image of one corner of Lateral calibration standard used for finding offset between different magnifications
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ReferenceMirrorFlatnessError
Reference mirror surface error map for a chosen magnification (objective and zoom tube combination)
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ObjectiveFocusOptimization
Effect of focus on roughness for selected samples with varying roughness values
0
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Part 1 Part 2 Part 3 Part 4 Part 5 Part 6
Low (< 40 nm) Medium (41 - 80 nm) High (81 - 120 nm)
Pa (n
m)
After 50x Focus Pa (nm) After Defocus Pa (nm) After Refocus Pa (nm)