2014
DOI: 10.1016/j.apradiso.2014.03.017
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The design of a multisource americium–beryllium (Am–Be) neutron irradiation facility using MCNP for the neutronic performance calculation

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Cited by 14 publications
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“…This is disadvantageous when large samples need to be activated since the radiation intensity will be disproportionate closest to the source, as the sample periphery becomes activated at a slower rate than the parts of the sample closest to the source. An important property of 241 AmBe is its high ratio of thermal neutrons in its characteristic spectrum, compared to that of other radioisotopic sources [17].…”
Section: Ambe the Neutron Yield Of A 241mentioning
confidence: 99%
“…This is disadvantageous when large samples need to be activated since the radiation intensity will be disproportionate closest to the source, as the sample periphery becomes activated at a slower rate than the parts of the sample closest to the source. An important property of 241 AmBe is its high ratio of thermal neutrons in its characteristic spectrum, compared to that of other radioisotopic sources [17].…”
Section: Ambe the Neutron Yield Of A 241mentioning
confidence: 99%