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authorThomas White <taw@physics.org>2015-06-18 15:53:03 +0200
committerThomas White <taw@physics.org>2015-06-19 13:30:31 +0200
commita0aca50f1150a664a141ea4a39ca065aef743202 (patch)
tree60baebf369f0c971b21c3baa0a92c27996828ccf /doc/man/process_hkl.1
parent1062513f7ecb912a50aef9559270a8218c0bacde (diff)
Update docs
Diffstat (limited to 'doc/man/process_hkl.1')
-rw-r--r--doc/man/process_hkl.12
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