Difference between revisions of "JB Absolute theta"
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== Beam == | == Beam == | ||
| − | I | + | I performed an MCNP simulation of a D2O target subject to an 10.5 MeV end-point bremsstrahlung beam. A mock-up of our entire neutron detector array is included in the simulation. Detector physics is modeled by applying a detection threshold in terms of light output (MeVee), which is equal to the typical MeVee produced by 0.5 MeV neutrons within the scintillator. |
| − | A Cf252 source was also simulated, allowing me to | + | |
| + | A Cf252 source was also simulated, allowing me to apply the exact same analysis technique to simulation and experimental data . | ||
[[File:2NCorrD2OExpvsMCNP.png|600px]] | [[File:2NCorrD2OExpvsMCNP.png|600px]] | ||
Revision as of 06:44, 9 November 2017
Beam
I performed an MCNP simulation of a D2O target subject to an 10.5 MeV end-point bremsstrahlung beam. A mock-up of our entire neutron detector array is included in the simulation. Detector physics is modeled by applying a detection threshold in terms of light output (MeVee), which is equal to the typical MeVee produced by 0.5 MeV neutrons within the scintillator.
A Cf252 source was also simulated, allowing me to apply the exact same analysis technique to simulation and experimental data .
MCNP-POLIMI
Below is an MCNP-POLIMI simulation of a cylindrical D20 target (axis length = 2"; dia. = 0.75") subject to a bremsstrahlung photon beam with an end point of 10.5MeV. The plot below shows the relative distribution of neutron direction cosines w.r.t. the incident photon beam. All neutrons are from the photodisintegration of D20 and the direction cosine is taken as neutrons exit the target geometry.
