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Metrology Scanning profilometry (contact and non-contact) SEM AFM Contact angle 1

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Page 1: Metrology - University of Kansas

MetrologyScanning profilometry (contact and non-contact)

SEM

AFM

Contact angle

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Page 2: Metrology - University of Kansas

By Emok - Own work, GFDL, https://commons.wikimedia.org/w/index.php?curid=3783176

Contact Profilometry

A tip, called a stylus, is scanned over the surface of a sample with a given applied force and measures variations in the surface topology

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Page 3: Metrology - University of Kansas

• Stylus radius ranges from 20 nm

to 50 mm. (Typical 2-15 mm)

• Can measure heights ranging

from 10 nm to 1 mm.

• Extremely quick measurement

• Very common tool – present in

most cleanrooms

• Typically only scans a line

across the sample

• 3D imaging possible, but at

much lower resolution

Contact

Profilometry

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Contact Profilometry Data

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Page 5: Metrology - University of Kansas

Optical Profilometry

• Non-contact profilometer based on

optical feedback

• Much faster than contact (stylus)

based profilometry

• 3D mapping is more practical than

with a stylus based system

• Lateral resolution ranges from a few

microns to sub micron

Most common types of optical

profilometers

• Optical Interference

• Confocal Aperture

• Focus Detection

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Page 6: Metrology - University of Kansas

http://www.laserfocusworld.com/articles/print/volume-46/issue-1/features/optical-surface-profiling.html

Interference Profilometry

• Sample moves up and down

• Light from sample and a

reference mirror recombine at

the detector to produce

interference fringes.

• Height at which the

interferogram is in best focus is

recorded for each point

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The optical path difference = height difference

Each transition (dark/light) =1/2 wavelength

Page 7: Metrology - University of Kansas

Confocal Aperture

http://www.nanoscience.com/technology/optical-profiler-technology/confocal-wli-pattern-projection-focus-detection/confocal-profilometry/ 7

1. Illumination wavelength is 409

nm.

2. 0.5 nm linear scale module (Z-

resolution).

3. Resolution Repeatability, Z-axis:

≤10 nm.

4. Smallest Feature Detection: ≤10

nm.

5. Spatial Resolution (X/Y): ≤ 180

nm.

6. Motorized Stage: X-Y-Z ; 100 mm

x 100 mm range min.

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Optical Resolution

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Practical limit obtained when imaging very small objects

by magnification

diffraction causes blurring of objects when imaging

smaller than 200-500 nm

(diffraction limit)

“broadening” of a point caused by diffraction is

known as the “point spread function, PSF” ()

x-y = (0.61 )/( sin())

= refractive index medium

= half-cone angle of focused light

=𝜆

2 𝑁𝐴

Page 9: Metrology - University of Kansas

Optical Profilometry Examples

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Page 10: Metrology - University of Kansas

Stylus versus Optical Profilometry

http://www.filmetrics.com/opticalprofilers/profilm3d-vs-stylus10

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Scanning Electron Microscopy

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Page 12: Metrology - University of Kansas

http://www.ammrf.org.au/myscope/sem/background/

Light Microscope versus SEM

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Scanning Electron Microscopy (SEM)

X-rays

SEM detected electrons

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1. Tungsten filament

2. Solid state crystal (Cerium hexaboride or Lanthanum

hexaboride)

3. Low energy (50 eV)

4. Image formed by inelastic scattering

Page 14: Metrology - University of Kansas

Secondary Electron Image

1. Secondary electrons are knocked out of the sample by the primary electron beam.2. Escape Depth = ~2 nm. 3. SE image is an image of surface topography

i.e. reveals topographical contrast.

SE generation indicates the shape, edges produce more electrons – better contrast, looks brighter

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Back Scattered Electrons• BSE are primary electrons that scatter back out of the sample.

• BSE signal arises from a much deeper depth than secondary electrons

• Images show less surface topology, but more atomic number contrast

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Page 16: Metrology - University of Kansas

SE vs BSESecondary

Electron Image

Backscattered

Electron Image

Solder on a circuit board16

Page 17: Metrology - University of Kansas

ChargingA buildup of negative charge on a specimen irradiated with an electron beam.

http://www.ammrf.org.au/myscope/sem/practice/principles/troubleshooting.phphttp://classes.mst.edu/civeng120/extra/galena_rose/index.html

Sample preparation considerations:• In a traditional SEM, non-conductive samples should

be coated with metal, carbon to prevent charging (a thin conductive film)

• An environmental SEM (ESEM) can be used to prevent charging (allows wet samples visualization, water vapor is an imaging gas)

gaseous secondary electron detector

https://itg.beckman.illinois.edu/microscopy_suite/equipment/downloads/how_it_works.pdf17

Page 18: Metrology - University of Kansas

Charging

http://www.ammrf.org.au/myscope/sem/practice/principles/troubleshooting.phphttp://classes.mst.edu/civeng120/extra/galena_rose/index.html

Sample preparation considerations:

• In a traditional SEM, non-conductive samples should be coated with metal to prevent charging

• An environmental SEM can also be used to prevent charging

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Atomic Force Microscopy

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Page 20: Metrology - University of Kansas

https://en.wikipedia.org/wiki/Atomic-force_microscopy#/media/File:Atomic_force_microscope_block_diagram.svg

AFM Schematic

Tapping mode

• Most common imaging mode

• Tip oscillates at its resonant frequency and

taps along the surface

• Helps to prevent damage to the tip/sample

Contact mode

• A constant force is applied between the tip

and the surface.

• The tip will move up and down to track the

surface topology and keep the force

constant

• Can cause damage to the tip/sample

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Page 21: Metrology - University of Kansas

https://en.wikipedia.org/wiki/Atomic-force_microscopy#/media/File:AFM_(used)_cantilever_in_Scanning_Electron_Microscope,_magnification_1000x.JPG

AFM Tips

• Wide variety of AFM tips:

• Different materials (Si, Si4N3)

• Different spring constants

• Different geometries

• Different surface chemistries

• AFM tips are much sharper

(end radius of <10 nm) than

profilometer tips

Tips with high aspect ratios may be required to

image nanochannels

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AFM of Nanochannels

FIB milled nanochannel

Resin stamp produced from FIB milled nanochannel

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Advantages of AFM• Creates a 3D map of surface

• Can calculate surface roughness

• Many other types of experiments possible (force curves, imaging

in fluid, electrical measurements, etc.)

• Can achieve atomic lateral resolution and sub nm resolution in z

Graphenehttp://blogs.lt.vt.edu/sustainablenano/2015/09/28/atomic-force-microscopy-application-in-nanoscience/

Disadvantages• Scans take much longer than

SEM (5-10 minutes per image)

• AFM artifacts can cause

distortions

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AFM Artifacts• The AFM image is a combination of surface topology and tip geometry.

Tip is not sharp enough for the feature.

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https://upload.wikimedia.org/wikipedia/commons/7/71/Afm_artifact2.pnghttp://www.nanophys.kth.se/nanophys/facilities/nfl/afm/fast-scan/bruker-help/Content/Service%20and%20Apps/Troubleshooting/AFM%20Image%20Quality.htm

AFM Artifacts

Tip is wider than

the feature.

Tip is dirty.

25Dull/dirty tip

Double tip

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http://www.ramehart.com/images/ca2.jpg

Contact Angle

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Page 27: Metrology - University of Kansas

http://www.ramehart.com/images/ca2.jpg

Contact Angle

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ssg = ssl + slg • cos q

θ = contact angleσsg = surface free energy of the solidσsl = interfacial tension between liquid and solidσlg = surface tension of the liquid

Young’s Equation

Page 28: Metrology - University of Kansas

Contact Angle for Treated COC Surfaces

Can we add functionality by UV/Ozone treatment?-C-OH -COOH

Data from Colleen O’Neil, Soper lab

Polyethylene (PE)Cyclic Olefin Copolymer (COC)

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Page 29: Metrology - University of Kansas

Thank You!

Any Questions?

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