[ Identification | Description | Input parameters | Output parameters | Links ]
Principle: The optimizer first (step 1) computes neutron state parameter limits passing in the Source_Optimizer, and then (step 2) records a Reference source as well as the state (at Source_Optimizer position) of neutrons reaching Monitor. The optimized source is defined as a fraction of the Reference source plus the distribution of 'good' neutrons reaching the Monitor. The optimization then starts (step 3), and focuses new neutrons on the Monitor_Optimizer. In fact it changes 'bad' neutrons into 'good' ones (that reach the Monitor), acting on their position, spin and divergence or velocity. The overall Monitor flux is kept during process. The energy and polarisation distributions are kept during optimization as far as possible during optimisation. The optimization method considers that all neutron parameters - (x,y), (vx,vy,vz) or (vx/v2,vy/v2,v2), (sx,sy,sz) or (sx/s2,sy/s2,s2) - are independent. Options: The optimized source can be computed regularly ('continuous' option) or only once ('not continuous'). The time spent in steps 1 and 2 can be reduced for a shorter optimization ('auto'). The neutrons passing during steps 1 and 2 can be smoothed for a better neutron weight distribution ('smooth' option). Source_optimizer can be placed at any position where you want to act on the flux, for instance just after the source. Monitor_Optimizer should be placed at position(s) to optimize. I prefer to put one just before the sample. Default parameters bins, step, and keep are 10, 10% and 10% respectively. The option string can be empty (""), which stands for default configuration that works fine in usual cases: options="continuous optimization, auto mode, smooth, SetXY+SetDivV+SetDivS" Possible options are continuous for continuous source optimization (default). verbose displays optimization process (debug purpose). auto uses the shortest possible 'step 1' and 'step 2' and sets 'step' value as required (default). smooth remove possible spikes generated in steps 1 and 2 (default is smooth). unactivate to unactivate the Optimizer. no or not revert next option bins=[value=10] set the Number of cells for sampling neutron states step=[value=10] Optimizer step in % of simulation. keep=[value=10] Percentage of initial source distribution that is kept file=[name] Filename where to save optimized source distributions (no file is generated if not given. Default ext. is .src) SetXY Keywords to indicate what may be changed during SetV optimisation. Default is position, divergence and spin SetS direction ("SetXY+SetDivV+SetdivS"). Choosing the speed SetDivV or spin optimization (SetV or SetS) may modify the energy SetDivS or polarisation distribution (norm of V and S) as the three components are then independent. Parameters bins, step and keep can also be entered as optional parameters. EXAMPLE: I use the following settings optim_s = Source_Optimizer(options="please be clever") (same as empty) (...) Monitor_Optimizer(xmin=-0.05, xmax=0.05, ymin=-0.05, ymax=0.05, optim_comp = "optim_s") A good optimization needs to record enough non optimized neutrons on Monitor during step 2. Typical enhancement in computation speed is by a factor 20. This component usually works well. NOTE: You must be aware that in some cases (SetV and SetS), the optimization might sligtly afect the energy or spin distribution of the source. The optimizer tries to do its best anyway. Also, some 'spikes' may sometime appear in monitor signals in the course of the optimization, coming from non-optimized neutrons with original weight. The 'smooth' option minimises this effect (on by default).
|bins||1||Number of cells for sampling neutron states.||10|
|step||0-100||Optimizer step in percent of simulation.||0.1|
|keep||0-100||Percentage of initial source distribution that is kept.||0.1|
|options||str||string of options. See Description||0|
[ Identification | Description | Input parameters | Output parameters | Links ]Generated automatically by McDoc, Peter Willendrup <firstname.lastname@example.org> / Wed Nov 23 21:27:13 2022