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| author | Thomas White <taw@physics.org> | 2018-02-27 16:48:23 +0100 |
|---|---|---|
| committer | Thomas White <taw@physics.org> | 2018-02-27 17:12:42 +0100 |
| commit | df26c722cdcc68f4b3dcc09976ad0075b8e65537 (patch) | |
| tree | 03418df0c8667c81c7b1751f97c3e5db08ba4a5b /doc | |
| parent | 6c0f047d2e87f939ed84bcf961b2b0361cbe6d55 (diff) | |
partialator: Tidy up old log files, and add --no-logs
Diffstat (limited to 'doc')
| -rw-r--r-- | doc/man/partialator.1 | 5 |
1 files changed, 5 insertions, 0 deletions
diff --git a/doc/man/partialator.1 b/doc/man/partialator.1 index decaa07c..980af00f 100644 --- a/doc/man/partialator.1 +++ b/doc/man/partialator.1 @@ -132,6 +132,11 @@ Reject crystals if the absolute values of their relative Debye-Waller ("B") fact .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. +.PD 0 +.IP \fB--no-logs\fR +.PD +Do not write the extensive log files needed for plotting contour maps and spectrum graphs. This makes the process a lot faster, but you probably do want these logs to check that post-refinement is working reasonably. + .SH PARTIALITY MODELS The available partiality models are: |