|
|
|
|
![]() |
![]() |
![]() | ||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||
|
About McStas Download Documentation |
14.120 The MCViNE_ConstantEnergyTransfer McStas ComponentIsotropic scatterer with a fixed energy transfer.
Identification
DescriptionEvery scattered neutron loses exactly the energy E (E<0: gains) and leaves in a uniformly random direction over 4pi. Useful for testing and resolution studies. Transport (same as MCViNE HomogeneousNeutronScatterer): on the first passage the neutron is forced to scatter at a uniformly chosen depth, weighted by path length, attenuation exp(-(mu+sigma)x) and the scattering coefficient; on exit it is attenuated by exp(-(mu+sigma)L_out). With order>1 further scatterings are sampled analogically (truncated exponential). With p_transmit>0 that fraction of events is kept as the attenuated direct beam. mu(v) = absorption_coefficient*2200/v. Events for which the kernel cannot scatter (kinematically forbidden) are absorbed. Geometry: box (xwidth,yheight,zdepth), cylinder (radius,yheight), hollow cylinder (+thickness) or sphere (radius only). All vectors (Q, targets, reciprocal vectors, atom positions) are in the component’s local frame. Uses the shared runtime share/mcvine-lib.h/.c. Example: MCViNE_ConstantEnergyTransfer(E=10, scattering_coefficient=10, radius=0.01, yheight=0.05)
Input parametersParameters in boldface are required; the others are optional.
Links
|
|||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||
| ||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||