diff options
| author | Thomas White <taw@physics.org> | 2020-10-23 14:55:55 +0200 |
|---|---|---|
| committer | Thomas White <taw@physics.org> | 2020-10-23 16:36:10 +0200 |
| commit | b2972c07cbd053651493f8efdb4981c663c29287 (patch) | |
| tree | c3f905bd3f02e7c22d9d9ad3e5126eeedf351526 /doc/man/partialator.1 | |
| parent | 2c51b20e1a7570255fc702632611578edbc6f92d (diff) | |
partialator(1): Add missing partiality models
Diffstat (limited to 'doc/man/partialator.1')
| -rw-r--r-- | doc/man/partialator.1 | 8 |
1 files changed, 8 insertions, 0 deletions
diff --git a/doc/man/partialator.1 b/doc/man/partialator.1 index 515f66d7..601a2c44 100644 --- a/doc/man/partialator.1 +++ b/doc/man/partialator.1 @@ -196,6 +196,14 @@ This model is the same as that described in Acta Cryst. D71 (2015) p1400. .PD Fix all partialities at 1. +.IP \fBoffset\fR +.PD +Treat the radiation as perfectly monochromatic, and calculate the partiality as exp(-t^2/R^2), where t is the excitation error and R is the reflection radius (taking mosaicity into account). This model is similar to that used by XDS. + +.IP \fBggpm\fR +.PD +An analytical overlap integral modelling the reflection profiles as Gaussian functions, and the radiation spectrum as a sum of Gaussians. + .SH USAGE CASES .IP "Merging without scaling, partialities or post-refinement:" |