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The sensitivity of a typical collimator instrument is proportional to a square root of the detector area (instead of being linearly proportional to the detector area) because the internal background increases as the detector area increases.
This is because the numerator is always proportional to the square of the detector area and the shot noise variance is always proportional to the detector area.
Hence, if shot noise is dominant, then the SNR is proportional to the detector area.
The detector area of each imaging method is shown in white color in d – g.
Collimating the beam to the detector area improves the energy resolution by about 10%.
In this paper, the characteristics of the THz-wave detector area will be discussed.
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This can be mitigated by using very small active detector areas (d_{B}).
The results of the model calculations indicate that detector areas of several square meters are required.
Because of factors like insufficient detector areas, ambiguous interaction models and intrinsic fluctuations in the processes, the progress in this field has been very slow.
A new 3D Proton Induced X-Ray Emission Tomography (PIXE-T) and Scanning Transmission Ion Microscopy Tomography (STIM-T) simulation software has been developed in Java and uses NVIDIA™ Common Unified Device Architecture CUDAA) to calculate the X-ray attenuation for large detector areas.
The source and detector areas can be overlapped or be coincided.
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