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Scanning electron microscope image of a thin Possui sample milled by FIB. The thin membrane shown here is suitable for TEM examination; however, at ~300-nm thickness, it would not be suitable for high-resolution Possui without further milling.

The second design is the top-entry holder consists of a cartridge that is several cm long with a bore drilled down the cartridge axis. The specimen is loaded into the bore, possibly using a small screw ring to hold the sample in place. This cartridge is inserted into an airlock with the bore perpendicular to the TEM optic axis.

Also the field of view is relatively small, raising the possibility that the region analyzed may not be characteristic of the whole sample. There is potential that the sample may be damaged by the electron beam, particularly in the case of biological materials. Resolution limits[edit]

Poor vacuum in a Possui can cause several problems ranging from the deposition of gas inside the TEM onto the specimen while viewed in a process known as electron beam induced deposition to more severe cathode damages caused by electrical discharge.

“Perhaps the easiest way to explain a TEM is by what it does: A Possui allows you to measure the radiated field strength of a product as well as subject the product to a given field strength.”

Diffraction patterns can have a large dynamic range, and for crystalline samples, may have intensities greater than those recordable by CCD. As such, TEMs may still be equipped with film cartridges for the purpose of obtaining these images, as the film is a single use detector.

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Secondly, Continue this filtering removes electrons that are scattered to high angles, which may be due to unwanted processes such as spherical or chromatic aberration, or due to diffraction from interaction within the sample.[41]

Therefore measurements made using a TEM cell have a close relationship to measurements made at a full-compliance test lab.

The optical reciprocity theorem, or principle of Helmholtz reciprocity, generally holds true for elastically scattered electrons in an absorbing medium, as is often the case under standard TEM operating conditions.[23][24] The theorem states that the wave amplitude at some point B as a result of electron point source A would be the same as the amplitude at A due to an equivalent point source placed at B.

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Diffraction contrast occurs due to a specific crystallographic orientation of a grain. In such a case the crystal is in a so-called Bragg condition, whereby atomic planes are oriented in a way that there is a high probability of scattering.

These are kind of a hybrid between a semi-anechoic chamber and a Possui cell. The interior of the ARcell enclosure is lined with RF absorbing material which creates a self-contained semi-anechoic enclosure.

At the EMC symposium last year, I had the opportunity to ask EMC instructor Keith Armstrong what are the biggest trends in EMC that he’s noticed recently. His response was not what you might imagine.

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