2017
DOI: 10.1016/j.nucet.2017.02.001
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Thickness optimization of Sn–Pb alloys for experimentally measuring mass attenuation coefficients

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Cited by 26 publications
(2 citation statements)
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“…The experimental error in the values of / m r associated with this measuring time does not exceed 5%. For better experimental results for measuring mass attenuation coefficient, the thickness must be optimized by keeping the product of linear attenuation coefficient and thickness of sample between 0.5 and 0.7 [40].…”
Section: Methodsmentioning
confidence: 99%
“…The experimental error in the values of / m r associated with this measuring time does not exceed 5%. For better experimental results for measuring mass attenuation coefficient, the thickness must be optimized by keeping the product of linear attenuation coefficient and thickness of sample between 0.5 and 0.7 [40].…”
Section: Methodsmentioning
confidence: 99%
“…The density ρ of alloy samples measured by Archimedes' principle is further used to compute primarily the optimum thickness range of the shielding materials. The optimum thickness range was derived from the product of the linear attenuation coefficient μ and the thickness t of the sample that lies in the range m   t 0.5 0.7 [39]. The optimum thickness range of a shielding substance allows single photon interaction and accurate measurement of mass attenuation coefficient values experimentally.…”
Section: Optimum Thickness Rangementioning
confidence: 99%