SQ (Module)
Overview
The SQ
module calculates the atomic structure factors, $S(Q)$, via Fourier transform of a source set of radial distribution functions. The total structure factor, $F(Q)$, is also generated through summation of the atomic partials.
The required radial distribution functions must be calculated by an
RDF
module and referenced using the SourceRDFs
keyword.
The
RDF
module dictates the target configurations from which the $g(r)$, and hence the $S(Q)$, are generated - as such, the SQ
module does not target any configurations itself. If Bragg scattering is to be explicitly included, a source
bragg
module can be specified with the IncludeBragg
keyword.
Description
Basic Theory
For a configuration containing $N$ distinct atom types there are $\frac{1}{2}N(N+1)$ unique partial structure factors $S_{ij}(Q)$, where $i$ and $j$ are the $i^{th}$ and $j^{th}$ atom type respectively. In the Faber-Ziman formalism, these partial structure factors are related to the radial distribution function via Fourier transform as follows:
$$ S_{ij}(Q) = 4\pi\rho \int_0^\inf [g_{ij}(r)-1] \frac{sin(Qr)}{Qr} r^2 dr $$
where $g_{ij}(r)$ is the radial distribution function between atom types $i$ and $j$, and $\rho$ is the atomic number density of the system. The full structure factor $F(Q)$, is the sum of the partials weighted by the atomic concentrations $c$ of the atom type involved:
$$ F(Q) = \sum^N_{i,j,i \geq j} [2-\delta_{ij}] c_i c_j S_{ij}(Q) $$
Instrumental Broadening
Any broadening arising from instrumental effects (i.e. instrumental broadening) can be applied to the calculated $S(Q)$ with the QBroadening
keyword. Any modules that apply weighting factors (e.g.
NeutronSQ
) to the structure factors generated by SQ
will therefore also contain this broadening. If data from different sources with differing broadening functions is required, then multiple SQ
modules must be used.
Bragg Scattering
Intensity information from a Bragg module
calculation can be incorporated into the calculate S(Q) and F(Q) by setting the IncludeBragg
keyword to the name of the relevant module. Intensities will be broadened according to the BraggQBroadening
keyword - note that the QBroadening
keyword has no effect on the broadening of Bragg intensities.
Keywords
Targets
Keyword | Arguments | Default | Description |
---|---|---|---|
SourceRDFs |
Module |
– | Required Source RDF module from which to take $g(r)$ and transform to $S(Q)$. |
Control
Keyword | Arguments | Default | Description |
---|---|---|---|
Averaging |
n |
5 |
Number of historical partial sets to combine into final partials |
AveragingScheme |
AveragingScheme |
Linear |
Weighting scheme to use when averaging partials |
QDelta |
qdelta |
0.01 |
Step size in $Q$ for Fourier transform. |
QMax |
qmax |
30.0 |
$Q_{max}$ limit of Fourier transform. |
QMin |
qmin |
0.01 |
$Q_{min}$ limit of Fourier transform. |
QBroadening |
Function1D |
None |
Broadening function to convolve in the Fourier transform. |
WindowFunction |
WindowFunction |
None |
Window function to apply in the Fourier transform. |
Bragg Keywords
Keyword | Arguments | Default | Description |
---|---|---|---|
IncludeBragg |
[Module ] |
– | Source
bragg
module from which to take and incorporate reflection information. The reflections are broadened according to the function specified by the BraggQBroadening keyword. |
BraggQBroadening |
Function1D |
None |
Broadening function to apply to Bragg reflection data. |
Export
Keyword | Arguments | Default | Description |
---|---|---|---|
Export |
bool |
false |
Whether to save partials to disk after calculation. A separate file is written for each individual atomic partial between types $i$ and $j$, as well as the summed total. |