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skoupy_r
2024-03-15 16:52:43 +01:00
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About.md

@ -9,7 +9,7 @@ Several restrictions and limitations described are based on comparison of set va
Electron probe shape can be reconstructed during iterative reconstruction, but its size (probe window) is limited by
```math
w_{full} = \frac{\lambda \cdot CL_{eff}}{d_{eff}} [reference?]
w_{full} = \frac{\lambda \cdot CL_{eff}}{d_{eff}} [ref]
```
where $`\lambda`$ is electron wavelength, $`CL_{eff}`$ the effective detector camera length and $`d_{eff}`$ the effective real space pixel size (including binning).
@ -28,7 +28,7 @@ where $`w_{full}`$ is probe window and $`\alpha_{corr}`$ the real probe semi-ang
Pixel size in reconstructed image made by iterative methods is not given by real space electron probe sampling density, but by maximal angular cover of the detector. It can be calculated by
```math
pix_{ptycho} = \frac{\lambda CL_{eff}}{d_{eff} N_{eff}/2} [reference]
pix_{ptycho} = \frac{\lambda CL_{eff}}{d_{eff} N_{eff}/2} [ref]
```
where $`\lambda`$ is electron wavelength, $`CL_{eff}`$ the effective detector camera length, $`N_{eff}`$ the number of detector's effective pixels (considering binning) and $`d_{eff}`$ the effective real space pixel size (considering binning).