Reflections on the Projection of Ions in APT 245
Figure 8. Effect of the projection model on the reconstruction of a thin layer normal to the direction of analysis for a simulated geometry of R=90nm and α=14°. The ideally reconstructed layer is depicted as dashed black lines. The equidistant projection model (blue) gives satisfactory results, whereas pseudo-stereographic model needs adjustment of the parameters with respect to the physical parameters. ICF, image compression factor.
CONCLUSIONS
In conclusion, we would like to point that the pseudo- stereographic projection was introduced in the early imple- mentation of the tomographic reconstruction protocol, and, for the small field-of-view instruments, was working fine. Although it has been extended to wide angle instruments, it should in fact only be considered as a small-angle approxi- mation of the real projections. The azimuthal equidistant model, although not ideal, has a validity domainmuch closer to the modern instruments setup. In summary, we have shown that
∙ the ion projection in APT and FIM is best described by an azimuthal equidistant projection;
∙ the azimuthal equidistant is expected to work on a broad range of specimen geometries;
∙ this projection was shown to be not only more accurate, but also more robust than the pseudo-stereographic projection when it comes to errors on, e.g., the position of the center of the projection;
∙ the implementation of a protocol based on such a projection is simple and could easily be generalized.
ACKNOWLEDGMENT
Dr. M.P. Moody, Dr. L.T. Stephenson, Dr. R.K.W. Marceau, Dr.D.Haley,Dr.T.C. Peterson,Dr.
F.Vurpillot,
Dr.B.P.Geiser, and Dr. D.J. Larson are all thanked for fruitful discussions over the years. The authors extend their gratitude to Shyeh Tjing Cleo Loi who developed and performed the Lorentz-based simula- tions that have enabled part of this work. B.G. is grateful for the support from Prof. S.P. Ringer and Prof. J.M. Cairney as well as the Australian Microscopy & Microanalysis Research Facility at the University of Sydney, where some of the data presented herein was obtained. Dr. Eric Jägle and Liang Wu are acknowledged for the provision of the pure Al data set obtained
on the Cameca LEAP 5000. For the record, the authors owe Dr. Jägle an alcoholic beverage to thank him for letting the authors use the data set. Finally, B.G. is grateful for the support provided by Prof. Raabe and the group atMPIE.
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