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| author | Thomas White <taw@physics.org> | 2015-06-30 11:18:18 +0200 |
|---|---|---|
| committer | Thomas White <taw@physics.org> | 2015-06-30 11:18:18 +0200 |
| commit | c6be0929ad9e4cb7289215a5ef9f48444314e0f0 (patch) | |
| tree | 11c48a39f4222ab39cebed7e270440ae5482686c /doc/man/partialator.1 | |
| parent | f0a96798696fe08a4c45a8ea41a8175faf13774a (diff) | |
Fix mistakes in documentation
Diffstat (limited to 'doc/man/partialator.1')
| -rw-r--r-- | doc/man/partialator.1 | 2 |
1 files changed, 1 insertions, 1 deletions
diff --git a/doc/man/partialator.1 b/doc/man/partialator.1 index 32bd433c..3f24a34f 100644 --- a/doc/man/partialator.1 +++ b/doc/man/partialator.1 @@ -93,7 +93,7 @@ Include a reflection in the output only if it appears at least least \fIn\fR tim .PD 0 .IP \fB--push-res=\fIn\fR .PD -Merge reflections which are up to \fIn\fR nm^-1 higher than the apparent resolution limit of each individual crystal. \fIn\fR can be negative to merge \fIlower\fR than the apparent resolution limit. The default is \fB--rescut=0\fR - note that this is different to the default behaviour of \fBprocess_hkl\fR. +Merge reflections which are up to \fIn\fR nm^-1 higher than the apparent resolution limit of each individual crystal. \fIn\fR can be negative to merge \fIlower\fR than the apparent resolution limit. The default is \fBpush-res=0\fR - note that this is different to the default behaviour of \fBprocess_hkl\fR. .SH PARTIALITY MODELS |