2013 3rd International Conference on Advancements in Nuclear Instrumentation, Measurement Methods and Their Applications (ANIMM 2013
DOI: 10.1109/animma.2013.6727884
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POLITRANI, a new toolkit to simulate organic scintillator pulses

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Cited by 2 publications
(3 citation statements)
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“…The energy deposition of a proton is therefore converted in MeV equivalent electron (MeVee), which is the energy that an electron would release by slowing down in the plastic scintillator to produce the same light pulse. A previous study concerning BC-420 plastic scintillators [9] gives the following conversion in case for recoil protons: E (MeVee) = 0.0364En 2 + 0.125En and in case of recoil carbon nuclei [5] [10] the relationship is: E (MeVee) = 0.02En where En is the energy deposited by the neutron, in MeV. The only consider here fast neutron reactions inducing recoil protons in plastic scintillators.…”
Section: Thresholds Settings For Plastic Scintillatorsmentioning
confidence: 99%
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“…The energy deposition of a proton is therefore converted in MeV equivalent electron (MeVee), which is the energy that an electron would release by slowing down in the plastic scintillator to produce the same light pulse. A previous study concerning BC-420 plastic scintillators [9] gives the following conversion in case for recoil protons: E (MeVee) = 0.0364En 2 + 0.125En and in case of recoil carbon nuclei [5] [10] the relationship is: E (MeVee) = 0.02En where En is the energy deposited by the neutron, in MeV. The only consider here fast neutron reactions inducing recoil protons in plastic scintillators.…”
Section: Thresholds Settings For Plastic Scintillatorsmentioning
confidence: 99%
“…Indeed, large detection volumes are needed to preserve coincidence counting statistics and therefore, a large number of PSD scintillators should be implemented as their size is limited. Actually, the difference between neutron and gamma ray pulse tails is not preserved in large PSD scintillators due to light multiple scattering [5] [6]. Finally, a large array of small (maximum 5 inches) PSD scintillators would increase the cost to a similar level as 3 He detectors, not to mention flammability and toxicity of organic liquid scintillators.…”
Section: Introductionmentioning
confidence: 99%
“…Indeed, large detection solid angles and volumes are needed to preserve coincidence counting statistics and therefore, a large number of PSD scintillators should be implemented as their size is limited. Actually, the difference between neutron and gamma-ray pulse tails is not preserved in large PSD scintillators due to multiple light scattering [12], [13]. Finally, a large array of small (maximum 5 in) PSD scintillators would increase the cost to a similar level as 3 He detectors.…”
Section: Introductionmentioning
confidence: 99%