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authorThomas White <taw@physics.org>2020-02-05 13:45:59 +0100
committerThomas White <taw@physics.org>2020-02-05 13:45:59 +0100
commit6c265f4ab4635c378b1a2ee3a654899470124d4d (patch)
tree8475d499e5907d8da369cf888cc6af7a32cefdbd /doc
parent5a645c757aead2b62e75e982587a03dbb21fcd54 (diff)
Fix manual typo
Diffstat (limited to 'doc')
-rw-r--r--doc/man/ambigator.12
1 files changed, 1 insertions, 1 deletions
diff --git a/doc/man/ambigator.1 b/doc/man/ambigator.1
index 4daaeb72..f0bb9014 100644
--- a/doc/man/ambigator.1
+++ b/doc/man/ambigator.1
@@ -29,7 +29,7 @@ If the ambiguity operator is known (or, equivalently, the actual and apparent sy
The default behaviour is to compare each crystal to every other crystal. This leads to a computational complexity proportional to the square of the number of crystals. If the number of crystals is large, the number of comparisons can be limited without compromising the algorithm much. In this case, the crystals to correlate against will be selected randomly.
-By default, the reflections will be compared and correlated in three resolution bins: up to 10, 10-2.5 and about 2.5 Angstrom. You can override this by using \fB--highres\fR and \fB--lowres\fR, in which case only one resolution bin will be used for all reflections.
+By default, the reflections will be compared and correlated in three resolution bins: up to 10, 10-2.5 and above 2.5 Angstrom. You can override this by using \fB--highres\fR and \fB--lowres\fR, in which case only one resolution bin will be used for all reflections.
.SH OPTIONS