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| author | Thomas White <taw@physics.org> | 2020-10-23 14:55:55 +0200 |
|---|---|---|
| committer | Thomas White <taw@physics.org> | 2020-10-23 14:55:55 +0200 |
| commit | 6e566883571bde2adeabaa83af286f9cc4e17c6d (patch) | |
| tree | 6feaa28fb75601c9ba86dd24b17d38a37942d618 /doc | |
| parent | 532af7ccb4fb427546f6938247c1b77791fe8d26 (diff) | |
partialator(1): Add missing partiality models
Diffstat (limited to 'doc')
| -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:" |