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author | Thomas White <taw@physics.org> | 2018-02-26 17:21:50 +0100 |
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committer | Thomas White <taw@physics.org> | 2018-02-27 17:12:42 +0100 |
commit | bd5d2ec01be4aef4731498424fe777e3cdb797ef (patch) | |
tree | 612e8a1da5a3e51ac8ca4b0c391818eaf8d8f936 /doc/man | |
parent | 989b96e3970d94f4480d05229dceaed8d7f33d0d (diff) |
Add --force-bandwidth and --force-radius
Diffstat (limited to 'doc/man')
-rw-r--r-- | doc/man/partialator.1 | 6 |
1 files changed, 6 insertions, 0 deletions
diff --git a/doc/man/partialator.1 b/doc/man/partialator.1 index c9ef85a0..0a5b78ba 100644 --- a/doc/man/partialator.1 +++ b/doc/man/partialator.1 @@ -151,6 +151,12 @@ Specify the indexing ambiguity operator. Example: \fB--operator=k,h,-l\fR. .IP If you prefer, you can specify the ambiguity operator by specifying the apparent symmetry using \fB-w\fR. +.PD 0 +.IP \fB--force-bandwidth=\fIbw\fR +.IP \fB--force-radius=\fIR\fR +.PD +Set the X-ray bandwidth or initial profile radius for all crystals before proceeding. Bandwidth is given as a fraction, i.e. \fB--force-bandwidth=0.0013\fR means 0.13 percent (approximate FWHM). Radius is given in nm^-1. + .SH PARTIALITY MODELS The available partiality models are: |