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| author | Thomas White <taw@bitwiz.org.uk> | 2013-10-03 15:34:07 -0700 |
|---|---|---|
| committer | Thomas White <taw@bitwiz.org.uk> | 2013-10-03 15:34:07 -0700 |
| commit | 7182d68c5b532e6863b25c4e5e6f82a514703103 (patch) | |
| tree | 3460ee4af2d2719721e357b4954280b9b3b716d7 /doc/man/partialator.1 | |
| parent | e9c8ae21d54fbf5f70da4d5a6c9b58136cbaa1fa (diff) | |
Update man page
Diffstat (limited to 'doc/man/partialator.1')
| -rw-r--r-- | doc/man/partialator.1 | 25 |
1 files changed, 25 insertions, 0 deletions
diff --git a/doc/man/partialator.1 b/doc/man/partialator.1 index 38292975..15992646 100644 --- a/doc/man/partialator.1 +++ b/doc/man/partialator.1 @@ -84,10 +84,35 @@ Refine and scale patterns against the reflections in \fIfilename\fR, instead of comparing them against each other. .PD 0 +.IP "\fB-m\fR \fImodel\fR" +.IP \fB--model=\fR\fImodel\fR +.PD +Specify the partiality model. See the list below for possible choices. + +.PD 0 .IP "\fB-j\fR \fIn\fR" .PD Run \fIn\fR analyses in parallel. +.SH PARTIALITY MODELS + +The available partiality models are: + +.IP \fBsphere\fR +.PD +The volume of intersection between a sphere centered on each reciprocal lattice +point, and the part of reciprocal space excited by the Ewald sphere taking into +account the finite bandwidth and convergence angle. A Lorentz factor will also +be used, proportional to the distance between the limiting Ewald spheres. + +For a fully description including diagrams, see T. A. White et al., Acta Cryst. +D69 (2013) p1231-1240. + +.IP \fBunity\fR +.PD +Fix all partialities at 1, and use no Lorentz factor at all. + + .SH BUGS This program is \fIexperimental\fR in this version of CrystFEL. It is not |