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authorThomas White <taw@physics.org>2013-11-06 17:05:57 +0100
committerThomas White <taw@physics.org>2013-11-06 17:05:57 +0100
commit41a8d87549ae245d30940943fe814c9434e88b12 (patch)
tree1cb98083f1acb1f934e5510999c910f3fc6d2931 /doc
parente6508cf8ffb1a686edfe2cda33a0580bb7bd78ec (diff)
get_hkl: Add anisotropic truncation
Diffstat (limited to 'doc')
-rw-r--r--doc/man/get_hkl.18
1 files changed, 8 insertions, 0 deletions
diff --git a/doc/man/get_hkl.1 b/doc/man/get_hkl.1
index 4bdfc822..9697b4ec 100644
--- a/doc/man/get_hkl.1
+++ b/doc/man/get_hkl.1
@@ -67,6 +67,14 @@ Only reflections in the input list which also appear in \fIfilename\fR will be w
.PD
The intensities of the reflections will be multiplied by their symmetric multiplicities according to the point group of the input list.
+.SH APPLYING A RESOLUTION CUTOFF
+.PD 0
+.IP \fB--cutoff-angstroms=\fR\fIn\fR
+.IP \fB--cutoff-angstroms=\fR\fIn1,n2,n3\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.
+
.SH AUTHOR
This page was written by Thomas White.