2004
DOI: 10.1016/j.apradiso.2004.02.008
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Determination of 4.438MeV γ-ray to neutron emission ratio from a 241Am–9Be neutron source

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Cited by 49 publications
(20 citation statements)
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“…The 4.4 MeV peak of Be-based neutron generators can often be used to discriminate these sources from fission sources. The yield of the 4.4 MeV photon per neutron emission is 0.60 [10]. This photon emission also explains the higher absolute efficiency of the NaI portal monitor with the AmBe source as compared to the 252 Cf source.…”
Section: Detection Efficiencymentioning
confidence: 76%
“…The 4.4 MeV peak of Be-based neutron generators can often be used to discriminate these sources from fission sources. The yield of the 4.4 MeV photon per neutron emission is 0.60 [10]. This photon emission also explains the higher absolute efficiency of the NaI portal monitor with the AmBe source as compared to the 252 Cf source.…”
Section: Detection Efficiencymentioning
confidence: 76%
“…These particles are produced via 9 Be(α, n) 12 C reactions, where the α particle is created in radioactive decays of 241 Am. In about 60 % of the cases, the carbon nucleus is produced in an excited state, and emits a 4.4 MeV gamma in addition to the neutron [53]. To get a background-free neutron capture sample, this high energy gamma is used to do a delayed coincidence search with the neutron capture.…”
Section: Delayed Neutron Detection Efficiencymentioning
confidence: 99%
“…Conversely, the main drawback of 241 Am-Be source is its relative high gamma background due to 4.43 MeV [12] emitted by 12 C, product of the reaction (a, n) on Beryllium. For the prototype developed in this work, a second component of the background of less importance, which must be taken into account, is due to 2.23 MeV prompt gamma emitted during hydrogen neutron capture.…”
Section: Introductionmentioning
confidence: 97%