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| -rw-r--r-- | doc/man/partialator.1 | 25 |
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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 |