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| author | Thomas White <taw@physics.org> | 2014-03-03 17:08:32 +0100 |
|---|---|---|
| committer | Thomas White <taw@physics.org> | 2014-03-03 17:09:00 +0100 |
| commit | 89862e5d5bc8814cfc483d9e9e50fbe7937803b4 (patch) | |
| tree | e53de3cc820156ffb3806a5bbc0d7ca7610261c7 /doc/man/process_hkl.1 | |
| parent | 5208f447990f163ae23f8313eb4f4045d5b95afd (diff) | |
process_hkl: Add --max-adu
Diffstat (limited to 'doc/man/process_hkl.1')
| -rw-r--r-- | doc/man/process_hkl.1 | 6 |
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 |