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IV. Pseudo-Voigt and Other Functions


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Combination Functions

These combine different functions in an attempt to get the "best of both worlds" as far as peak shape is concerned. The combination can be by convolution (e.g. the Voigt function) or by simple addition (e.g. pseudo-Voigt which is a close approximation to the Voigt function). For example the latter case could take the form:

I(2θ) = IhklL (2θ − 2θ0) + (1 − η) G (2θ − 2θ0) ]

where, respectively, L (2θ − 2θ0) and G (2θ − 2θ0) represent suitably normalised Lorentz and Gaussian functions, and η (the "Lorentz fraction") and (1 − η) represent the fractions of each used. The main features of combination functions are:

Split Functions

These are used when the peak is noticeably asymmetric. Basically a given function is doctored so that it has a parameter with one value for the left hand side and another value for the right hand side of the peak. For example with the Gaussian function, the peak width, through FWHM, could be set at one value Hleft for 2θ < 2θ0 and at another Hright for 2θ > 2θ0 . The degree of asymmetry can then be said to be measured by the magnitude of   HleftHright / (Hleft + Hright ),   the sign indicating whether skewing is towards higher or lower angles.

One-dimensional Fourier Series

Fourier series are good at reproducing a given arbitrary shape provided sufficient terms in the series are taken. Once the series is determined it can be easily manipulated and convoluted in various mathematical operations. However this can be computationally expensive and therefore this approach is less useful for applications, such as structure refinement, where the peak shape needs to be computed many times over, however it is used widely for the study of microstructure.

Non-analytical Functions

A quite different approach is to dispense with the use of mathematical functions and instead set up a list of parameters (e.g. a generic look-up table) which describes the peak shape. The main features are:


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Author(s): Paul Barnes
Simon Jacques
Martin Vickers