diff options
| author | Thomas White <taw@physics.org> | 2013-11-06 17:05:57 +0100 |
|---|---|---|
| committer | Thomas White <taw@physics.org> | 2013-11-06 17:05:57 +0100 |
| commit | 41a8d87549ae245d30940943fe814c9434e88b12 (patch) | |
| tree | 1cb98083f1acb1f934e5510999c910f3fc6d2931 /doc | |
| parent | e6508cf8ffb1a686edfe2cda33a0580bb7bd78ec (diff) | |
get_hkl: Add anisotropic truncation
Diffstat (limited to 'doc')
| -rw-r--r-- | doc/man/get_hkl.1 | 8 |
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. |