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Formulas
Several restrictions and limitations described are based on comparison of set values with calculated limits. These are based on following formulas.
Reconstruction probe window
Electron probe shape can be reconstructed during iterative reconstruction, but its size (probe window) is limited by
where \lambda
is electron wavelength, CL_{eff}
the effective detector camera length and d_{eff}
the effective real space pixel size (including binning).
Maximal usable defocus
Electron probe grows in size with induced defocus accordingly to the probe semi-angle. For proper reconstruction, the probe has to fit into probe window with some safety margins (recommended is to use half of the window). Maximum defocus is so given by
where w_{full}
is probe window and \alpha_{corr}
the real probe semi-angle.
Pixel size in the reconstructed image
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
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).
Scattering angle to real space spacing
As we know CTF in angle units, we have to recalculate its shape to real space spacing in a sample. It can be calculated by
where \lambda
is electron wavelength and \theta
is the scattering angle
Tested packages
Proper widgets layout was tested in JupyterLab 4.0.8 and Python 3.11.5. The code was tested with packages:
- Numpy version 1.26.2
- Scipy version 1.11.4
- Plotly version 5.18.0
- Pandas version 2.1.1
- IPython version 7.31.1
- Ipywidgets version 8.0.4