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author | Thomas White <taw@physics.org> | 2019-06-25 17:11:09 +0200 |
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committer | Thomas White <taw@physics.org> | 2019-06-25 17:24:44 +0200 |
commit | 9c97f8f5c0aacec6d4098f1bea89e8b08f7169fe (patch) | |
tree | 3f013ef5c5595942268adf3446d1515df8c65fc8 /doc/man | |
parent | 53f71ffbc5b0202e872bd606c91130d99145b783 (diff) |
partial_sim: Add --template-stream
Diffstat (limited to 'doc/man')
-rw-r--r-- | doc/man/partial_sim.1 | 6 |
1 files changed, 6 insertions, 0 deletions
diff --git a/doc/man/partial_sim.1 b/doc/man/partial_sim.1 index 72655758..d7b91040 100644 --- a/doc/man/partial_sim.1 +++ b/doc/man/partial_sim.1 @@ -148,6 +148,12 @@ Set the central photon energy, in eV, for the incident beam. The default is \fB .IP \fB--really-random\fR .PD Seed the random number generator using the kernel random number generator (/dev/urandom). This means that truly random (although not "cryptographically random") numbers will be used for the orientation and crystal size, instead of the same sequence being used for each new run. + +.IP "\fB--template-stream=\fImy.stream\fR" +.PD +Get the crystal cell parameters, orientations and the reflections to calculate from \fImy.stream\fR. This allows you to re-calculate partial intensities using new beam parameters. There must only be one crystal per chunk in the template. If more than one thread is used (see \fB-j\fR), note that there is no guarantee that the order of crystals in the output stream will match that of \fImy.stream\fR. + + .SH AUTHOR This page was written by Thomas White. |