Transmission electron microscopy (TEM) – diffraction

About this technique


Crystalline materials scatter electrons by Bragg diffraction. This results in the formation of patterns wherein the symmetries and intensities provide information on the crystalline structure of the material. The most frequently used diffraction mode on a transmission electron microscope (TEM) is selected area diffraction. Here an aperture is used to select the region of interest. This may be as small as 0.5 µm in diameter. Putting the microscope into diffraction mode results in a pattern being displayed on the screen. Single crystal regions of specimen, where the electron beam lies parallel to a low index crystallographic direction will result in simple spot patterns. The separation of the spots can be used to determine the d-spacing of the crystal (with an accuracy of about 1 %) and the angles between, and the relative spacings of, the spots can be used to determine the zone axis of the crystal. Where two phases are selected by the aperture (e.g. a precipitate within a matrix), then the composite pattern arising from the two lattices can be used to determine the orientation relationship between the phases. Where polycrystalline materials are examined, ring diffraction patterns are obtained. Here the ring radii may be converted into d-spacings.

Electron diffraction is a powerful adjunct to the imaging and spectroscopy capabilities of a TEM. Generally, one already knows a great deal about the material before carrying out diffraction. The limited accuracy and precision of electron diffraction when compared with X-ray diffraction for example, makes it difficult to identify phases with diffraction alone, in the absence of supporting information like composition.

There are a number of more specialised electron diffraction techniques. Nanobeam diffraction uses a very fine parallel probe of just a few namometres to generate diffraction information. This is useful for investigating discrete nanoparticles or localised regions such as interfacial layers. Convergent beam diffraction uses a highly convergent beam focused to a very small spot. This technique can be used for space group determination, precise orientation, foil thickness and a number of other highly specialised techniques.

Output examples

[TEM-diff_01_TF.jpg]
Selected area diffraction pattern showing intense spots from the Mg matrix as well a weaker reflections from the precipitates in an alloy.


Contact an expert

The University of Sydney
Dr Hongwei Liu
T: 02 9351 3995
E: hongwei.liu@sydney.edu.au

The University of Western Australia
Prof. Martin Saunders
T: 08 6488 8092
E: martin.saunders@uwa.edu.au

The University of New South Wales
Dr Mark Lockrey
T: 02 9385 6390
E: m.lockrey@unsw.edu.au

Curtin University
Dr Zakaria Quadir
T: 08 9266 1026
E: Zakaria.Quadir@curtin.edu.au

Deakin University
Dr Pavel Cizek
T: 03 5227 3242
E: pavel.cizek@deakin.edu.au

University of Wollongong
Dr Gilberto Casillas-Garcia
T: 02 4221 3272
E: gilberto@uow.edu.au

University of Wollongong
Dr James Bouwer
T: 02 4221 3281
E: jbouwer@uow.edu.au

Monash University
Dr Laure Bourgeois
T: 03 9905 5368
E: laure.bourgeois@monash.edu

The Australian National University
Dr Felipe Kremer
T: 02 6125 6553
E: felipe.kremer@anu.edu.au