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Resolution and FWHM in Two-dimensional Diffraction

The resolution of a two-dimensional detector is governed to a dominant extent by the PSF. This can be very well observed by the behaviour of the FWHM distribution of reflections over an image plate. The PSF of a standard image plate is roughly 300 pm. The projection A/ of the diffracted beam width d on the image plate in the case of a fully parallel beam is given by  [Pg.419]

Adding the FWHM resulting from the point spread contribution would lead to  [Pg.419]

As Equation (3) still holds Equation (4) would become  [Pg.420]

The detector resolution can be estimated as a convolution of the footprint with the PSF. Placing this in Equation (6) would lead to the following formula, again for an idealized non-tilted detector  [Pg.421]

As both the footprint and the PSF can be described by a Gaussian function the FWHM of their convolution is given by  [Pg.421]


See other pages where Resolution and FWHM in Two-dimensional Diffraction is mentioned: [Pg.419]   


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