1986
DOI: 10.1016/0306-4549(86)90105-2
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Penetration of 2.75 MeV γ-rays through shielding slabs of graphite, aluminium, steel and lead

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Cited by 7 publications
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“…This parameter is used when the experimental conditions are violated from those referred to as narrow beam or ideal geometry, thin attenuator and mono-energetic radiation source. The BFs may be determined by experiment [3,4], empirical formula [5], and simulation codes such as MCNP [6,7].…”
Section: Introductionmentioning
confidence: 99%
“…This parameter is used when the experimental conditions are violated from those referred to as narrow beam or ideal geometry, thin attenuator and mono-energetic radiation source. The BFs may be determined by experiment [3,4], empirical formula [5], and simulation codes such as MCNP [6,7].…”
Section: Introductionmentioning
confidence: 99%