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-rw-r--r--doc/man/compare_hkl.126
1 files changed, 14 insertions, 12 deletions
diff --git a/doc/man/compare_hkl.1 b/doc/man/compare_hkl.1
index 26ec7faf..1b4cdf4b 100644
--- a/doc/man/compare_hkl.1
+++ b/doc/man/compare_hkl.1
@@ -72,14 +72,14 @@ I1 and I2 are the intensities of the same reflection in both reflection lists.
.RE
.PD 0
-.IP \fB-u\fR
+.IP \fB--nshells=\fR\fIn\fR
.PD
-Fix scale factors to unity.
+Use \fIn\fR resolution shells. Default: 10.
.PD 0
-.IP \fB--nshells=\fR\fIn\fR
+.IP \fB-u\fR
.PD
-Use \fIn\fR resolution shells. Default: 10.
+Fix scale factors to unity.
.PD 0
.IP \fB--shell-file=\fIfilename\fR
@@ -104,12 +104,20 @@ Discard reflections with I/sigma(I) < \fIn\fR. Default: -infinity (no cutoff).
.PD 0
.IP \fB--rmin=\fR\fI1/d\fR
.PD
-Discard reflections with lower than this value of 1/d in m^-1.
+Low resolution cutoff, as 1/d in m<sup>-1</sup>. Use this or \fB--lowres\fR, but not both.
+
+.PD 0
+.IP \fB--lowres=\fR\fId\fR
+Low resolution cutoff in Angstroms. Use this or \fB--rmin\fR, but not both.
.PD 0
.IP \fB--rmax=\fR\fI1/d\fR
.PD
-Discard reflections with higher than this value of 1/d in m^-1.
+High resolution cutoff, as 1/d in m<sup>-1</sup>. Use this or \fB--highres\fR, but not both.
+
+.PD 0
+.IP \fB--highres=\fR\fId\fR
+High resolution cutoff in Angstroms. Use this or \fB--rmax\fR, but not both.
.PD 0
.IP \fB--intensity-shells\fR
@@ -118,12 +126,6 @@ Use intensity shells instead of resolution shells. The range of shells will sta
.sp
Because of the hardcoded factor of 1/5000, needed to avoid a very uneven distribution of the number of reflection pairs in each bin, you are advised not to draw strong conclusions from the results of using this option.
-.PD 0
-.IP \fB--shell-file=\fR\fIfilename\fR
-.PD
-Write the statistics in resolution shells to \fIfilename\fR.
-
-
.SH AUTHOR
This page was written by Thomas White.