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| author | Thomas White <taw@physics.org> | 2016-02-05 15:33:18 +0100 |
|---|---|---|
| committer | Thomas White <taw@physics.org> | 2016-02-05 15:33:18 +0100 |
| commit | 775afe633f3cc104b916bbf5f0b43c2225999d53 (patch) | |
| tree | b98c2fedf1e80b95a35f7695ec7b40ef96a046f1 | |
| parent | 0872486795f6235180a133a5ce89e7c98aa02107 (diff) | |
Update docs
| -rw-r--r-- | doc/man/partialator.1 | 7 |
1 files changed, 6 insertions, 1 deletions
diff --git a/doc/man/partialator.1 b/doc/man/partialator.1 index f184dd38..decaa07c 100644 --- a/doc/man/partialator.1 +++ b/doc/man/partialator.1 @@ -1,7 +1,7 @@ .\" .\" partialator man page .\" -.\" Copyright © 2012-2015 Deutsches Elektronen-Synchrotron DESY, +.\" Copyright © 2012-2016 Deutsches Elektronen-Synchrotron DESY, .\" a research centre of the Helmholtz Association. .\" .\" Part of CrystFEL - crystallography with a FEL @@ -127,6 +127,11 @@ Read a list of filenames, event IDs and dataset IDs from \fIfilename\fR. See th .PD Reject crystals if the absolute values of their relative Debye-Waller ("B") factors are more than \fIn\fR square Angstroms. The default is \fB--max-rel-B=100\fR. +.PD 0 +.IP \fB--output-every-cycle\fR +.PD +Write out the per-crystal parameters and reflection lists after every cycle of refinement, instead of only at the end. The intermediate reflection lists and parameter filenames will be prefixed with \fBiter\fIN\fB_\fR (note the trailing underscore), where \fIN\fR is the iteration number. If you use \fB--custom-split\fR, intermediate results will also be output for each custom dataset. + .SH PARTIALITY MODELS The available partiality models are: |