TY - JOUR
T1 - Active neutron interrogation
T2 - Experimental results from the PUNITA device
AU - Dubi, C.
AU - Ocherashvilli, A.
AU - Varasano, G.
AU - Yankovich, R.
AU - Bogucarska, T.
AU - Pedersen, B.
N1 - Publisher Copyright:
© 2020 Elsevier B.V.
PY - 2021/2/11
Y1 - 2021/2/11
N2 - The PUNITA device is a state-of-the-art active neutron interrogation facility, aimed to identify and quantify Special Nuclear Materials (SNM), by measuring induced fission neutrons. The source neutrons are generated by a powerful (D−T) tube, creating fast neutron pulses which are thermalized in a large graphite reflector. Due to the relative high detection efficiency, together with the strong thermal flux created, the PUNITA device holds some very favorable properties, and is capable of detecting SNM signature in fairly short measurement times. Yet, these exact same properties form interesting challenges and questions, due to self shielding effects and other spatial effects. In the present study, we introduce experimental results that differ from past experiments in four aspects: first, the mass range – up to 100 [gr] of 235U – is significantly larger than previous experiment. Second, as opposed to past experiments, not all samples have the same geometry and total U mass. Third, samples were repeatedly measured, to check the effect of source fatigue and source variance on the sampled values. Finally, a new mathematical formalism was used to quantify and account for the (D−T) source variance, and how it effects the sampled doubles rate.
AB - The PUNITA device is a state-of-the-art active neutron interrogation facility, aimed to identify and quantify Special Nuclear Materials (SNM), by measuring induced fission neutrons. The source neutrons are generated by a powerful (D−T) tube, creating fast neutron pulses which are thermalized in a large graphite reflector. Due to the relative high detection efficiency, together with the strong thermal flux created, the PUNITA device holds some very favorable properties, and is capable of detecting SNM signature in fairly short measurement times. Yet, these exact same properties form interesting challenges and questions, due to self shielding effects and other spatial effects. In the present study, we introduce experimental results that differ from past experiments in four aspects: first, the mass range – up to 100 [gr] of 235U – is significantly larger than previous experiment. Second, as opposed to past experiments, not all samples have the same geometry and total U mass. Third, samples were repeatedly measured, to check the effect of source fatigue and source variance on the sampled values. Finally, a new mathematical formalism was used to quantify and account for the (D−T) source variance, and how it effects the sampled doubles rate.
KW - Active neutron interrogation
KW - Neutron multiplicity counting
KW - Pulsed source
UR - http://www.scopus.com/inward/record.url?scp=85098455381&partnerID=8YFLogxK
U2 - 10.1016/j.nima.2020.164933
DO - 10.1016/j.nima.2020.164933
M3 - Article
AN - SCOPUS:85098455381
SN - 0168-9002
VL - 989
JO - Nuclear Instruments and Methods in Physics Research, Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
JF - Nuclear Instruments and Methods in Physics Research, Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
M1 - 164933
ER -