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-rw-r--r--doc/man/get_hkl.13
1 files changed, 3 insertions, 0 deletions
diff --git a/doc/man/get_hkl.1 b/doc/man/get_hkl.1
index 90637a8a..8d76c154 100644
--- a/doc/man/get_hkl.1
+++ b/doc/man/get_hkl.1
@@ -79,9 +79,12 @@ The intensities of the reflections will be multiplied by their symmetric multipl
.PD 0
.IP \fB--cutoff-angstroms=\fR\fIn\fR
.IP \fB--cutoff-angstroms=\fR\fIn1,n2,n3\fR
+.IP \fB--highres=\fR\fIn\fR
+.IP \fB--lowres=\fR\fIn\fR
.PD
In the first form, reflections with d (=lamba/2*sin(theta)) < \fIn\fR will be removed.
In the second form, anisotropic truncation will be performed with separate resolution limits \fIn1\fR, \fIn2\fR and \fIn3\fR along a*, b* and c* respectively. You must also specify \fB-p\fR or \fB--pdb\fR.
+The option \fB--lowres\fR will remove reflections with d > \fIn\fR. \fB--highres\fR is a synonym for \fB--cutoff-angstroms\fR.
.SH REINDEXING REFLECTIONS
.PD 0