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authorThomas White <taw@physics.org>2018-01-19 13:17:40 +0100
committerThomas White <taw@physics.org>2018-02-27 17:12:41 +0100
commit0f24c4fb9451f1c32fb89534b37bf7f804e37d99 (patch)
tree1a55f6dd1ba4c477e6aecd3141a298dcd420eb58 /doc
parentd813960912ddc76d5cff0501b4f7783c3eeca95d (diff)
indexamajig: Add --overpredict
Diffstat (limited to 'doc')
-rw-r--r--doc/man/indexamajig.15
1 files changed, 5 insertions, 0 deletions
diff --git a/doc/man/indexamajig.1 b/doc/man/indexamajig.1
index a434bf05..3f49701f 100644
--- a/doc/man/indexamajig.1
+++ b/doc/man/indexamajig.1
@@ -409,6 +409,11 @@ Show detailed information about reflection integration when \fIcondition\fR is m
.PD
When \fBrescut\fR is in the integration method, integrate \fIn\fR nm^-1 higher than the apparent resolution limit of each individual crystal. If \fBrescut\fR is not used, this option has no effect. \fIn\fR can be negative to integrate \fIlower\fR than the apparent resolution limit. The default is \fB--push-res=0\fR, but note that the default integration method does \fInot\fR include \fBrescut\fR, so no per-pattern resolution cutoff is used. Note that you can also apply this cutoff at the merging stage using \fBprocess_hkl --push-res\fR.
+.PD 0
+.IP \fB--overpredict\fR
+.PD
+Over-predict reflections. This is needed to provide a buffer zone when using post-refinement, but makes it difficult to judge the accuracy of the predictions because there are so many reflections. It will also reduce the quality of the merged data if you merge without partiality estimation.
+
.SH OUTPUT OPTIONS
.PD 0