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. 2017 Oct 25;3(1):15. doi: 10.1186/s40679-017-0048-z

Fig. 4.

Fig. 4

Comparison of the CPU/GPU implementations of the PRISM and multislice algorithms described in this work. A 100 × 100 × 100 Å amorphous carbon cell was divided slices of varying thickness and sampled with progressively smaller pixels in real space corresponding to digitized probes of array size 256 × 256, 512 × 512, 1024 × 1024, and 2048 × 2048, respectively. Two different PRISM simulations are shown, a more accurate case where the interpolation factor f=4 (left), and a faster case with f=16 (right). The multislice simulation is the same for both columns. Power laws were fit of the form A+Bqmaxn where possible. The asymptotic power laws for higher scattering angles are shown on the right of each curve