Electron microscopy
Read Tim Palucka's pages on the history of electron microscopy:
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The electron microscope is integral to characterization of materials.
Maybe more than 10,000 electron microscopes are in use across most
disciplines in the natural sciences. In the electron microscope
a beam of electrons is focused upon a target specimen. Information
may be gathered from electrons transmitted through the specimen,
from Bragg diffracted electrons, from Auger electrons, from characteristic
x-rays, and from the charge absorbed by the specimen. An explanation
of the workings of the electron microscopy at three levels (elementary,
high school, college) can be found on the Iowa
State Materials Science and Engineering Department's website
(from where the image on the left is also taken).
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The first operational electron microscope was presented by Ernst
Ruska and Max Knoll in 1932, and 6 years later Ruska had a first version
on the market. In 1986 Ruska received a Nobel Prize in physics for his
"fundamental work in electron optics and for the design of the first
electron microscope". The following table gives a basic outline of
the history of the electron microscope by decades.
Year
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Specimens
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Application/development
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Instrumentation/theory
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Resolution
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1940s |
Replicas
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- surfaces
- slip steps
- extracted particles
- fractography
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- 50kV, single condenser
- little or no theory; a first basic theory of
electron microscopy was published in 1949 by Heidenreich.
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~10nm |
1950s |
Thin foils:
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- defects
- phase transitions
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- 100kV
- contrast theory developed.
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~0.5-2nm |
1960s |
- metals
- semiconductors
- ceramics
- minerals
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- Dynamic in-situ studies
- substructure of solids
- radiation damage
- microdiffraction
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- high voltage electron
microscopes (Toulouse: 1.2 and 3MeV)
- scanning electron microscopes
- accessories for in-situ studies
- controlled experiments
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- 0.3nm (transmission)
- ~15-20nm (scanning)
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1970s |
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- High resolution imaging
- lattice imaging
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- Analytical transmission electron microscopy
- scanning transmission electron microscopy
- energy dispersive x-ray spectra
- electron energy loss spectroscopy
- commercial high voltage electron microscopy
(0.4-1.5MeV)
- high resolution imaging theory
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- 0.2nm (transmission)
- 7nm (standard scanning)
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1980s |
virtually all materials |
- atomic resolution in close-packed solids
- surface imaging
- small particles
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- commercial medium-voltage high-resolution/analytical
electron microscopy (300-400kV)
- improved analytical capabilities
- energy filtering imaging
- ultra-high vacuum microscopes
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- 0.15nm (transmission)
- 5nm (scanning at 1kV)
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1990s |
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- fast computation for image simulation
- alloy design
- nanostructures
- integrated digital scanning and image processing
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- surface atomic microscopy
- orientation imaging microscopy
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- 0.1nm (transmission)
- 3nm (scanning at 1kV)
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2000s |
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Most of the information in the above table
was taken from G. Thomas, "The impact of electron microscopy
on materials research", in Impact of Electron and
Scanning Probe Microscopy on Materials Research, edited
by Rickerby, Valdre, and Valdre, Kluwer:
1999; and from Vander Voort & Friel (eds.), Development
in Materials Characterization Technologies. The image
on the right is also taken from the latter (Figure 1, page
45) by permission of ASM
International, Materials Park, OH 44073-0002.
The use of the tree as a metaphor for the historical development
is interesting. It is certainly suggestive, and as such it
does not matter greatly whether the metaphor applies to all
facets. The tree metaphor points, of course, to the undisputable
fact that all specialized forms of electron microscopy could
not have emerged without the already existing earlier forms.
However, it also suggests parallels with an organism that
seems less accurate. The small branches and leaves could be
seen as having originated from many more sources than just
the original SEM. There was also no predisposition (such as
in a tree's DNA) to develop in just this fashion.
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