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author | Thomas White <taw@physics.org> | 2015-06-18 15:53:03 +0200 |
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committer | Thomas White <taw@physics.org> | 2015-06-19 13:30:31 +0200 |
commit | a0aca50f1150a664a141ea4a39ca065aef743202 (patch) | |
tree | 60baebf369f0c971b21c3baa0a92c27996828ccf /doc/man/process_hkl.1 | |
parent | 1062513f7ecb912a50aef9559270a8218c0bacde (diff) |
Update docs
Diffstat (limited to 'doc/man/process_hkl.1')
-rw-r--r-- | doc/man/process_hkl.1 | 2 |
1 files changed, 1 insertions, 1 deletions
diff --git a/doc/man/process_hkl.1 b/doc/man/process_hkl.1 index 0b795be1..632d624d 100644 --- a/doc/man/process_hkl.1 +++ b/doc/man/process_hkl.1 @@ -103,7 +103,7 @@ Merge crystals only if they diffract to beyond \fIn\fR Angstroms resolution. Th .PD 0 .IP \fB--push-res=\fIn\fR .PD -Integrate \fIn\fR nm^-1 higher than the apparent resolution limit of each individual crystal. \fIn\fR can be negative to integrate \fIlower\fR than the apparent resolution limit. The default is \fB--rescut=inf\fR, which means no resolution cutoff at all. +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=inf\fR, which means no resolution cutoff at all. .PD 0 .IP \fB--min-cc=\fIn\fR |