Hi Andy,
I would be more careful when trying to compare the shape function with small angle diffraction. There is a relationship between both entities but in all honesty i don't remember from the top of my head anymore.
if g(r) is the computed constraint before shape function subtraction and G(r) after subtraction then
G(r) = g(r) - 4*PI*r*N*T(r) where T(r) is the wide angle correlation function
as far as choosing the shape function parameters i would use the default in fullrmc and let it figure it out but if you think it's not doing a good job this is the intuition behind the parameters
- rmax: it must be bigger than the biggest distance in your atomic model. normally i would take more than the double of that maximum distance value (shannon sampling)
- rmin: i would set it to 0 or close to 0
- dr: you got to experiment because a too small or too big value will give you wiggles. knowing that no atoms are closer than 0.5A fullrmc considers this threshold
- qmin and qmax: the default parameters in fullrmc should cover a big range of particle sizes unless your system is millions of atoms huge.
I am not confident I should tell you what to chose this is up to you to look at the result and judge. Visual inspection is all what you need. At the end of the day you need to remember one very important thing, your experimental data is flattened visually using non physical shape functions. Fullrmc does things in more theoretical manner but this is being compared to experimentalist approach if you know what i mean.
don't sweat it, focus on analyzing the system after the simulation is done and testing different groups and moves upon those to get different configuration solutions...
best