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Reflections on the Projection of Ions in APT 243


Figure 6. Histograms of the average distance between simulated detected position and position predicted by the pseudo- stereographic (red) and equidistant (blue) models.


Figure 5. a: Distribution of the distance from the ion impact position to the center of the detector ρ as a function of the launch angle θ (dots) for various shank angles (see color bar) and speci- men radii in the range of 20–170 nm; superimposed are a linear regression (solid line) as well as the expected distribution based on the average image compression factor (dashed line). b: Ratio of the distribution obtained from the simulations to the linear regression (solid line) as well as that based on the average image compression factor.


simulation. The resulting histograms are shown on Figure 6 for the 97 simulations. The equidistant model has a dis- tribution of error localized around 0, whereas the pseudo- stereographic projection models introduces a significant systematic error, for a wide variety of sample geometries (shank angles varying from 2 to 14° and radii in the range of 20–170nm).


Figure 7. Same desorption map as in Figure 3 superimposed with the adjusted azimuthal equidistant (blue) and pseudo-stereographic (red) projections of 41 visible indexed crystallographic poles.


Projection and Orientation Adjustment


As the azimuthal equidistant angular projection accurately describes the actual projection in APT despite its very simple equations, it opens the way for automatic adjustments of the crystallographic features contained in the desorption maps, such as that of Figure 3, in order to accurately obtain the orientation of the specimen. This is what was done on Figure 7 where we superimposed the desorption image of a pure Al specimen, shown in Figure 3, with the predicted position of the crystallographic poles as well as zone axes based on the two projections (with ICFs


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