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author | Thomas White <taw@physics.org> | 2015-11-19 14:58:04 +0100 |
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committer | Thomas White <taw@physics.org> | 2015-11-19 14:59:52 +0100 |
commit | b07c8c3652d85f78262a776187e15ab41f098089 (patch) | |
tree | f7a2d7506a90272e050eef7bf2dc04af7effeda9 /doc | |
parent | a1d57905623ce56de278d204378494cdceef4970 (diff) |
partialator: Set default push-res to infinity
Not needed now that the scaling is more stable
Diffstat (limited to 'doc')
-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 ce3c7907..f184dd38 100644 --- a/doc/man/partialator.1 +++ b/doc/man/partialator.1 @@ -100,7 +100,7 @@ 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 \fBpush-res=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 \fB--push-res=inf\fR, which means no resolution cutoff at all. .PD 0 .IP \fB--start-after=\fR\fIn\fR |