Abstract
We review the use of restoration methods that recover the complex specimen exit wave from a suitably conditioned data set of high resolution transmission electron microscope images. Various levels of theory underlying the post-acquisition processing required are described together with the requirements for aberration measurement.
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Notes
- 1.
The origin of the use of real space order when describing an aberration coefficient originates from the ray-optical theory of Seidel aberrations which are described in terms of displacements of ray-path intersections with the image plane. As these displacements are proportional to the gradient of the wave aberration function, an nth order Seidel aberration corresponds to a term of order n + 1 in W. As an example, the image aberration for defocus is linear in angle and is hence described as a first-order aberration, whereas the image aberration for spherical aberration is cubic in angle and is hence described as a third-order aberration.
- 2.
As the apparent strength of the tilt coils is often sensitive to the condenser lens and objective lens pre-field excitation this must be constant between calibration and experiment.
- 3.
Current reversal centre alignment involves reversing the current of the objective lens but is no longer practicable with the strong lenses used in modern instruments.
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Haigh, S.J., Kirkland, A.I. (2012). High Resolution ExitWave Restoration. In: Vogt, T., Dahmen, W., Binev, P. (eds) Modeling Nanoscale Imaging in Electron Microscopy. Nanostructure Science and Technology. Springer, Boston, MA. https://doi.org/10.1007/978-1-4614-2191-7_3
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