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TEM constructed in 1931 
Von Ardenne, first STEM in 1938 by rastering the electron beam in a TEM 
Zworykin et al. 1942, first SEM for bulk samples 
1965 first commercial SEM by Cambridge Scientific Instruments 
Resolution at that time ~ 50 nm : Today < 1 nm 
Morphology only at that time : Today analytical instrument
It is a microscope that produces an image by using an electron beam that 
scans the surface of a specimen inside a vacuum chamber. 
What can we study in a SEM? 
•Topography and morphology 
•Chemistry 
•Crystallography 
•Orientation of grains 
•In-situ experiments: 
–Reactions with atmosphere 
–Effects of temperature 
“Easy” sample 
preparation!! 
“Big” samples!
AFM Cantilever Tip Ant Head Blood Cells 
Diamond Thin Film 
(Numerous Multifaceted Micro-crystals) 
Microstructure of a plain carbon 
steel that contains 0.44 wt% of 
carbon 
Calcium Phosphate 
Crystal
Magnification? 
Resolution?
 electron gun (filament) 
 electromagnetic optics 
 scan coils 
 sample stage 
 detectors 
 vacuum system 
 computer hardware and 
software (not trivial!!)
We want many electrons per time unit per area 
(high current density) and as small electron spot as 
possible 
Traditional guns: thermionic electron gun 
(electrons are emitted when a solid is heated) 
W-wire, LaB6-crystal 
Modern: field emission guns (FEG) (cold guns, a 
strong electric field is used to extract electrons) 
Single crystal of W, etched to a thin tip
Aperture in SEM: either to limit the amount of electrons or enhance contrast
Backscattered electron detector: 
(Solid-State Detector) 
Secondary electron detector: 
(Everhart-Thornley) 
Secondary electrons: Everhart-Thornley Detector 
Backscattered electrons: Solid State Detector 
X-rays: Energy dispersive spectrometer (EDS)
A detector placed within the column is known as an “in-lens” detector and 
produces a very different image compared to a conventionally located detector
 The SEM uses electrons instead of light to form an 
image. 
 A beam of electrons is produced at the top of the 
microscope by heating of a metallic filament. 
 The electron beam follows a vertical path through 
the column of the microscope. It makes its way through 
electromagnetic lenses which focus and direct the beam 
down towards the sample. 
 Once it hits the sample, other electrons 
( backscattered or secondary ) are ejected from the 
sample. Detectors collect the secondary or 
backscattered electrons, and convert them to a signal 
that is sent to a viewing screen similar to the one in an 
ordinary television, producing an image.
The incident electron beam is scattered in the sample, both elastically and inelastically 
This gives rise to various signals that we can detect (more on that on next slide) 
Interaction volume increases with increasing acceleration voltage and decreases with 
increasing atomic number
Incoming electrons 
Secondary electrons 
Backscattered 
electrons 
Auger electrons 
X-rays 
Cathodo-luminescence 
(light) 
Sample
 Diameter of the interaction volume is 
larger than the electron spot 
 resolution is poorer than the size of the 
electron spot
Generated from the collision between the incoming 
electrons and the loosely bonded outer electrons 
Low energy electrons (~10-50 eV) 
Only SE generated close to surface escape 
(topographic information is obtained) 
Number of SE is greater than the number of incoming 
electrons 
We differentiate between SE1 and SE2
A fraction of the incident electrons is retarded by 
the electro-magnetic field of the nucleus and if the 
scattering angle is greater than 180° the electron 
can escape from the surface 
High energy electrons (elastic scattering) 
Fewer BSE than SE 
We differentiate between BSE1 and BSE2
SE produces higher resolution images 
than BSE 
By placing the secondary electron 
detector inside the lens, mainly SE1 are 
detected 
Resolution of 1 – 2 nm is possible
Photons not electrons 
Each element has a fingerprint X-ray signal 
Poorer spatial resolution than BSE and SE 
Relatively few X-ray signals are emitted and the 
detector is inefficient 
 relatively long signal collecting times are needed
Thank You

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SEM Imaging Techniques Explained

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  • 2. TEM constructed in 1931 Von Ardenne, first STEM in 1938 by rastering the electron beam in a TEM Zworykin et al. 1942, first SEM for bulk samples 1965 first commercial SEM by Cambridge Scientific Instruments Resolution at that time ~ 50 nm : Today < 1 nm Morphology only at that time : Today analytical instrument
  • 3. It is a microscope that produces an image by using an electron beam that scans the surface of a specimen inside a vacuum chamber. What can we study in a SEM? •Topography and morphology •Chemistry •Crystallography •Orientation of grains •In-situ experiments: –Reactions with atmosphere –Effects of temperature “Easy” sample preparation!! “Big” samples!
  • 4. AFM Cantilever Tip Ant Head Blood Cells Diamond Thin Film (Numerous Multifaceted Micro-crystals) Microstructure of a plain carbon steel that contains 0.44 wt% of carbon Calcium Phosphate Crystal
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  • 8.  electron gun (filament)  electromagnetic optics  scan coils  sample stage  detectors  vacuum system  computer hardware and software (not trivial!!)
  • 9. We want many electrons per time unit per area (high current density) and as small electron spot as possible Traditional guns: thermionic electron gun (electrons are emitted when a solid is heated) W-wire, LaB6-crystal Modern: field emission guns (FEG) (cold guns, a strong electric field is used to extract electrons) Single crystal of W, etched to a thin tip
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  • 11. Aperture in SEM: either to limit the amount of electrons or enhance contrast
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  • 15. Backscattered electron detector: (Solid-State Detector) Secondary electron detector: (Everhart-Thornley) Secondary electrons: Everhart-Thornley Detector Backscattered electrons: Solid State Detector X-rays: Energy dispersive spectrometer (EDS)
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  • 17. A detector placed within the column is known as an “in-lens” detector and produces a very different image compared to a conventionally located detector
  • 18.  The SEM uses electrons instead of light to form an image.  A beam of electrons is produced at the top of the microscope by heating of a metallic filament.  The electron beam follows a vertical path through the column of the microscope. It makes its way through electromagnetic lenses which focus and direct the beam down towards the sample.  Once it hits the sample, other electrons ( backscattered or secondary ) are ejected from the sample. Detectors collect the secondary or backscattered electrons, and convert them to a signal that is sent to a viewing screen similar to the one in an ordinary television, producing an image.
  • 19. The incident electron beam is scattered in the sample, both elastically and inelastically This gives rise to various signals that we can detect (more on that on next slide) Interaction volume increases with increasing acceleration voltage and decreases with increasing atomic number
  • 20. Incoming electrons Secondary electrons Backscattered electrons Auger electrons X-rays Cathodo-luminescence (light) Sample
  • 21.  Diameter of the interaction volume is larger than the electron spot  resolution is poorer than the size of the electron spot
  • 22. Generated from the collision between the incoming electrons and the loosely bonded outer electrons Low energy electrons (~10-50 eV) Only SE generated close to surface escape (topographic information is obtained) Number of SE is greater than the number of incoming electrons We differentiate between SE1 and SE2
  • 23. A fraction of the incident electrons is retarded by the electro-magnetic field of the nucleus and if the scattering angle is greater than 180° the electron can escape from the surface High energy electrons (elastic scattering) Fewer BSE than SE We differentiate between BSE1 and BSE2
  • 24. SE produces higher resolution images than BSE By placing the secondary electron detector inside the lens, mainly SE1 are detected Resolution of 1 – 2 nm is possible
  • 25. Photons not electrons Each element has a fingerprint X-ray signal Poorer spatial resolution than BSE and SE Relatively few X-ray signals are emitted and the detector is inefficient  relatively long signal collecting times are needed
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