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authorThomas White <taw@physics.org>2014-04-08 17:03:00 +0200
committerThomas White <taw@physics.org>2014-04-08 17:08:53 +0200
commit1d6fdfc003f46ea5cf618459d215a032390afc15 (patch)
tree104745e8ef17bf9c022ed7512e73f2537adc4205 /doc/man/process_hkl.1
parent54176de692b7709e1148904089229f09758436f1 (diff)
process_hkl: Add --min-res
Diffstat (limited to 'doc/man/process_hkl.1')
-rw-r--r--doc/man/process_hkl.15
1 files changed, 5 insertions, 0 deletions
diff --git a/doc/man/process_hkl.1 b/doc/man/process_hkl.1
index e4a3dd8f..6aeaa2a8 100644
--- a/doc/man/process_hkl.1
+++ b/doc/man/process_hkl.1
@@ -114,6 +114,11 @@ Use a particular individual reflection intensity measurement only if it exceeds
.PD
Include reflections only if their peak values were less than \fIn\fR. That means, \fIn\fR is the saturation value of the detector. The default is infinity, i.e. no cutoff.
+.PD 0
+.IP \fB--min-res=\fR\fIn\fR
+.PD
+Merge crystals only if they diffract to beyond \fIn\fR Angstroms resolution. The default is zero, i.e. no cutoff. The resolution is taken from the diffraction_resolution_limit line in the stream.
+
.SH CHOICE OF POINT GROUP FOR MERGING