Parallelization of Atomic Image Reconstruction from Holograms
207
Fig. 1 Inverse mode of XFH
Fig. 2 Difference of optical path length in inverse mode
2.1 Reconstruction of Atomic Images
When the intensity I λ (l, θ, φ) measured at polar coordinate system k(l, θ, φ) on a
hologram on a sphere by incident X-ray of wave length λ, the position of an atom
in the sample can be calculated as follows.
207
Fig. 1 Inverse mode of XFH
Fig. 2 Difference of optical path length in inverse mode
2.1 Reconstruction of Atomic Images
When the intensity I λ (l, θ, φ) measured at polar coordinate system k(l, θ, φ) on a
hologram on a sphere by incident X-ray of wave length λ, the position of an atom
in the sample can be calculated as follows.