Package janus.format.endf.data.energydistrib encapsulates classes that represent energy distributions. These energy distributions include the probabilities of secondary particle emission at a given energy E’. This probability also depends on the energy E of the incident particle, and it is generally represented as p(E->E’). Energy distributions are imported from FILE 5 in ENDF format.
By default, the distribution is displayed for the first tabulated incident energy. A list of incident variables E at which the distribution is tabulated in the evaluation is given under Variables in the graphical user interface. For energies between tabulated values, the distribution is constructed by interpolating using the interpolation techniques specified in the evaluation.
Since the secondary energy distribution depends on the incident particle energy, the user may be interested in knowing how the probability of emitting a particle at a certain energy E’ depends on the incident energy E.
The energy distribution may be represented in the evaluation as the combination of partial energy distributions:
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where pk is the fractional probability and fk is the fractional distribution. The fractional probability is represented with class FractionalProbabilty. Class PartialEnergyDistribution and its subclasses maintain fractional distributions. For energy distributions of reactions with multiple incident particles or for delayed neutron distributions, each fractional probability and distribution may be displayed. These two pieces of information, the fractional probability and the distribution, are displayed in different tabs in the Renderer because they have unequal units.