Celeritas
0.5.0-56+6b053cd
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Sample energy loss from a Gaussian distribution. More...
#include <EnergyLossGaussianDistribution.hh>
Public Types | |
Type aliases | |
using | Energy = units::MevEnergy |
using | EnergySq = Quantity< UnitProduct< units::Mev, units::Mev > > |
Public Member Functions | |
CELER_FUNCTION | EnergyLossGaussianDistribution (Energy mean_loss, Energy bohr_stddev) |
Construct from mean/stddev. More... | |
CELER_FUNCTION | EnergyLossGaussianDistribution (Energy mean_loss, EnergySq bohr_var) |
Construct from distribution parameters. More... | |
CELER_FUNCTION | EnergyLossGaussianDistribution (EnergyLossHelper const &helper) |
Construct from helper-calculated data. | |
template<class Generator > | |
CELER_FUNCTION Energy | operator() (Generator &rng) |
template<class Generator > | |
CELER_FUNCTION auto | operator() (Generator &rng) -> Energy |
Sample energy loss according to the distribution. | |
Sample energy loss from a Gaussian distribution.
In a thick absorber, the total energy transfer is a result of many small energy losses from a large number of collisions. The central limit theorem applies, and the energy loss fluctuations can be described by a Gaussian distribution. See section 7.3.1 of the Geant4 Physics Reference Manual and GEANT3 PHYS332 section 2.3.
The Gaussian approximation is valid for heavy particles and in the regime \( \kappa = \xi / T_\textrm{max} > 10 \). Fluctuations of the unrestricted energy loss follow a Gaussian distribution if \( \Delta E > \kappa T_{max} \), where \( T_{max} \) is the maximum energy transfer (PHYS332 section 2). For fluctuations of the restricted energy loss, the condition is modified to \( \Delta E > \kappa T_{c} \) and \( T_{max} \le 2 T_c \), where \( T_c \) is the delta ray cutoff energy (PRM Eq. 7.6-7.7).
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Construct from mean/stddev.
This formulation is used internally by the Urban distribution.
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Construct from distribution parameters.
The mean loss is the energy lost over the step, and the standard deviation is the square root of Bohr's variance (PRM Eq. 7.8). For thick absorbers, the straggling function approaches a Gaussian distribution with this standard deviation.