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authorThomas White <taw@physics.org>2014-03-03 17:08:32 +0100
committerThomas White <taw@physics.org>2014-03-03 17:09:00 +0100
commit89862e5d5bc8814cfc483d9e9e50fbe7937803b4 (patch)
treee53de3cc820156ffb3806a5bbc0d7ca7610261c7 /doc
parent5208f447990f163ae23f8313eb4f4045d5b95afd (diff)
process_hkl: Add --max-adu
Diffstat (limited to 'doc')
-rw-r--r--doc/man/process_hkl.16
1 files changed, 6 insertions, 0 deletions
diff --git a/doc/man/process_hkl.1 b/doc/man/process_hkl.1
index d32d8b8f..427e3b75 100644
--- a/doc/man/process_hkl.1
+++ b/doc/man/process_hkl.1
@@ -109,6 +109,12 @@ Use a particular individual reflection intensity measurement only if it exceeds
.IP
\fBWARNING:\fR think very carefully before using this option. It will bias reflections towards more positive values, even where no signal exists, leading to a data set dominated by the background. This can invalidate some of the figures of merit for the merit for data quality while severely compromising the actual quality.
+.PD 0
+.IP \fB--max-adu=\fR\fIn\fR
+.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.
+
+
.SH CHOICE OF POINT GROUP FOR MERGING
One of the main features of serial crystallography is that the orientations of