|Status:||Resolved||Start date:||08 Aug 2016|
|Target version:||Sprint 34|
As first step to simulated AF spin arrangements on a square lattice I have tried to duplicate the simple single particle basis by doubling the unit cell parameters and using four particles in the basis.
The same intensity pattern for both simulations within numerical errors.
Different Bragg peak size and intensity as well as half order Bragg peaks that should be forbidden by selection rules.
This is an important issue that will be common for many AFM systems.
- Status changed from Sprint to Resolved
The problem described actually consists of two unrelated issues:
1) A normalization error in the 2D lattice interference function: this has been solved now
2) The violation of the selection rule: this is more subtle. Because of the way we handle finite-size effects (with a so-called decay function), the two cases considered above are not entirely equivalent. There is a selection rule appearing at exactly the peak positions that should be absent, but around it, there will be scattered intensity. This is a direct consequence of the decay function method and can not be cured ad hoc. The solution would be to provide another mechanism for finite-size effects that does not have this problem.