diff options
| author | Thomas White <taw@physics.org> | 2015-06-30 11:18:18 +0200 |
|---|---|---|
| committer | Thomas White <taw@physics.org> | 2015-06-30 11:18:18 +0200 |
| commit | c6be0929ad9e4cb7289215a5ef9f48444314e0f0 (patch) | |
| tree | 11c48a39f4222ab39cebed7e270440ae5482686c /doc | |
| parent | f0a96798696fe08a4c45a8ea41a8175faf13774a (diff) | |
Fix mistakes in documentation
Diffstat (limited to 'doc')
| -rw-r--r-- | doc/man/indexamajig.1 | 2 | ||||
| -rw-r--r-- | doc/man/partialator.1 | 2 | ||||
| -rw-r--r-- | doc/man/process_hkl.1 | 2 |
3 files changed, 3 insertions, 3 deletions
diff --git a/doc/man/indexamajig.1 b/doc/man/indexamajig.1 index a371180c..f6b7ba80 100644 --- a/doc/man/indexamajig.1 +++ b/doc/man/indexamajig.1 @@ -313,7 +313,7 @@ Show detailed information about reflection integration when \fIcondition\fR is m .PD 0 .IP \fB--push-res=\fIn\fR .PD -When \fBrescut\fR is in the integration method, integrate \fIn\fR nm^-1 higher than the apparent resolution limit of each individual crystal. If \fBrescut\fR is not used, this option has no effect. \fIn\fR can be negative to integrate \fIlower\fR than the apparent resolution limit. The default is \fB--rescut=0\fR. Note that you can also apply this cutoff at the merging stage using \fBprocess_hkl --push-res\fR. +When \fBrescut\fR is in the integration method, integrate \fIn\fR nm^-1 higher than the apparent resolution limit of each individual crystal. If \fBrescut\fR is not used, this option has no effect. \fIn\fR can be negative to integrate \fIlower\fR than the apparent resolution limit. The default is \fB--push-res=0\fR, but note that the default integration method does \fInot\fR include \fBrescut\fR, so no per-pattern resolution cutoff is used. Note that you can also apply this cutoff at the merging stage using \fBprocess_hkl --push-res\fR. .PD 0 .IP \fB--highres=\fIn\fR diff --git a/doc/man/partialator.1 b/doc/man/partialator.1 index 32bd433c..3f24a34f 100644 --- a/doc/man/partialator.1 +++ b/doc/man/partialator.1 @@ -93,7 +93,7 @@ Include a reflection in the output only if it appears at least least \fIn\fR tim .PD 0 .IP \fB--push-res=\fIn\fR .PD -Merge reflections which are up to \fIn\fR nm^-1 higher than the apparent resolution limit of each individual crystal. \fIn\fR can be negative to merge \fIlower\fR than the apparent resolution limit. The default is \fB--rescut=0\fR - note that this is different to the default behaviour of \fBprocess_hkl\fR. +Merge reflections which are up to \fIn\fR nm^-1 higher than the apparent resolution limit of each individual crystal. \fIn\fR can be negative to merge \fIlower\fR than the apparent resolution limit. The default is \fBpush-res=0\fR - note that this is different to the default behaviour of \fBprocess_hkl\fR. .SH PARTIALITY MODELS diff --git a/doc/man/process_hkl.1 b/doc/man/process_hkl.1 index 632d624d..072ee97d 100644 --- a/doc/man/process_hkl.1 +++ b/doc/man/process_hkl.1 @@ -103,7 +103,7 @@ Merge crystals only if they diffract to beyond \fIn\fR Angstroms resolution. Th .PD 0 .IP \fB--push-res=\fIn\fR .PD -Merge reflections which are up to \fIn\fR nm^-1 higher than the apparent resolution limit of each individual crystal. \fIn\fR can be negative to merge \fIlower\fR than the apparent resolution limit. The default is \fB--rescut=inf\fR, which means no resolution cutoff at all. +Merge reflections which are up to \fIn\fR nm^-1 higher than the apparent resolution limit of each individual crystal. \fIn\fR can be negative to merge \fIlower\fR than the apparent resolution limit. The default is \fB--push-res=inf\fR, which means no resolution cutoff at all. .PD 0 .IP \fB--min-cc=\fIn\fR |