From c6be0929ad9e4cb7289215a5ef9f48444314e0f0 Mon Sep 17 00:00:00 2001 From: Thomas White Date: Tue, 30 Jun 2015 11:18:18 +0200 Subject: Fix mistakes in documentation --- doc/man/indexamajig.1 | 2 +- 1 file changed, 1 insertion(+), 1 deletion(-) (limited to 'doc/man/indexamajig.1') diff --git a/doc/man/indexamajig.1 b/doc/man/indexamajig.1 index a371180c..f6b7ba80 100644 --- a/doc/man/indexamajig.1 +++ b/doc/man/indexamajig.1 @@ -313,7 +313,7 @@ Show detailed information about reflection integration when \fIcondition\fR is m .PD 0 .IP \fB--push-res=\fIn\fR .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--rescut=0\fR. Note that you can also apply this cutoff at the merging stage using \fBprocess_hkl --push-res\fR. +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--highres=\fIn\fR -- cgit v1.2.3