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| author | Thomas White <taw@physics.org> | 2015-07-07 11:57:33 +0200 |
|---|---|---|
| committer | Thomas White <taw@physics.org> | 2015-07-07 11:57:33 +0200 |
| commit | 270e3440f7fe3f8da5d31666c429179b9ae07798 (patch) | |
| tree | f4d2785a421575630b52892b752492db8ea81f20 /doc/man/partialator.1 | |
| parent | ca3e32582fd6b42fbc10778ded0db184db993e56 (diff) | |
Update docs
Diffstat (limited to 'doc/man/partialator.1')
| -rw-r--r-- | doc/man/partialator.1 | 10 |
1 files changed, 10 insertions, 0 deletions
diff --git a/doc/man/partialator.1 b/doc/man/partialator.1 index 3f24a34f..5c3c24bb 100644 --- a/doc/man/partialator.1 +++ b/doc/man/partialator.1 @@ -95,6 +95,16 @@ Include a reflection in the output only if it appears at least least \fIn\fR tim .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 \fBpush-res=0\fR - note that this is different to the default behaviour of \fBprocess_hkl\fR. +.PD 0 +.IP \fB--start-after=\fR\fIn\fR +.PD +Ignore the first \fIn\fR crystals in the input. The default is \fB--start-after=0\fR, i.e. start at the beginning. + +.PD 0 +.IP \fB--stop-after=\fR\fIn\fR +.PD +Stop processing after \fIn\fR crystals have been successfully read. The default is \fB--stop-after=0\fR, which means to process all the patterns from the start point to the end of the input (see \fB--start-after\fR). + .SH PARTIALITY MODELS The available partiality models are: |