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| author | Thomas White <taw@physics.org> | 2015-11-19 14:58:04 +0100 |
|---|---|---|
| committer | Thomas White <taw@physics.org> | 2015-11-19 14:59:52 +0100 |
| commit | b07c8c3652d85f78262a776187e15ab41f098089 (patch) | |
| tree | f7a2d7506a90272e050eef7bf2dc04af7effeda9 | |
| parent | a1d57905623ce56de278d204378494cdceef4970 (diff) | |
partialator: Set default push-res to infinity
Not needed now that the scaling is more stable
| -rw-r--r-- | doc/man/partialator.1 | 2 | ||||
| -rw-r--r-- | src/partialator.c | 2 |
2 files changed, 2 insertions, 2 deletions
diff --git a/doc/man/partialator.1 b/doc/man/partialator.1 index ce3c7907..f184dd38 100644 --- a/doc/man/partialator.1 +++ b/doc/man/partialator.1 @@ -100,7 +100,7 @@ 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 \fBpush-res=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 \fB--push-res=inf\fR, which means no resolution cutoff at all. .PD 0 .IP \fB--start-after=\fR\fIn\fR diff --git a/src/partialator.c b/src/partialator.c index 23f0c089..0c892a88 100644 --- a/src/partialator.c +++ b/src/partialator.c @@ -643,7 +643,7 @@ int main(int argc, char *argv[]) double max_adu = +INFINITY; char *sparams_fn = NULL; FILE *sparams_fh; - double push_res = 0.0; + double push_res = +INFINITY; gsl_rng *rng; int no_free = 0; char *csplit_fn = NULL; |