Calculation of the electron diffraction intensities using the multi-slice method
Abstract
For the calculation of the dynamical electron diffraction amplitude using the multi-slice method the slice thickness Δz must be carefully selected. Crystals with long lattice periods parallel to the electron beam must be subdivided into m projected potential slices (φm) of thickness ΔZm. Image simulations for Nb12O29 on the [100] orientation (a = 28.9 Å) at 200 kV for various slice thicknesses gave the best fit to the experimental image for Δz = 4.8 and 9.6 Å (6 and 3 slices pro unit cell), respectively. At higher accelerating voltage and better resolution, more beams contribute to the image; in this case Δz must be decreased. In addition (independently of the calculation method), it is shown that errors in interpretation also occur, if the relativistic mass effect is neglected in the scattering equations.
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Articles in the same Issue
- The thermal expansion of Na2CO3
- Crystal structure of a beryllium-potassium polyphosphate: BeK(PO3)3
- 4-Amino-2-bromo-6-methyl-5,6,7,8-tetrahydropyrido[2,3-d]-pyrimidine
- An X-ray analysis of anomalous dispersion effects, anharmonicity and thermal vibrations in gallium phosphide
- An empirical model of optical susceptibilities of crystals I. Refractivity in alkali halides
- An empirical model of optical susceptibilities of crystals II. Elasto-optical effect in alkali halides
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- Crystal structure of a mixed crystal containing 3-benzoyl-2-phenyl-furo[2,3-b]quinoxaline and 3-benzoyl-2-phenyl-thieno[2,3-b]quinoxaline
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- 10.1515/zkri.1986.177.3-4.171
- 10.1515/zkri.1986.177.3-4.177
- 10.1515/zkri.1986.177.3-4.185
- 10.1515/zkri.1986.177.3-4.201
- 10.1515/zkri.1986.177.3-4.211
- 10.1515/zkri.1986.177.3-4.219
- 10.1515/zkri.1986.177.3-4.229
- 10.1515/zkri.1986.177.3-4.237
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