2020
DOI: 10.1007/s10967-020-07046-3
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Measurement of the 238U(n,γ)239U reaction cross sections in the energy range of 2.0–5.0 MeV by using a neutron activation technique

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Cited by 1 publication
(2 citation statements)
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“…The 239 Np radionuclide is recognizable by the characteristic γ-rays of 106.1 keV, 228.2 keV, and 277.6 keV, whose intensities all surpass 10%. Nevertheless, the γ-rays at 277.6 keV were preferred over others in the calculations because the γ-rays at 106.1 keV and 228.2 keV are subjected to interference by the γ-rays at 103.2 keV and 228.2 keV originating from the fission products 153 Sm (T 1/2 = 46.284 h) and 132 Te (T 1/2 = 3.204 d), respectively [4][5][6]. In this experiment, the 197 Au (n, γ)…”
Section: B 238 U Neutron Capture Cross-section Calculationmentioning
confidence: 99%
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“…The 239 Np radionuclide is recognizable by the characteristic γ-rays of 106.1 keV, 228.2 keV, and 277.6 keV, whose intensities all surpass 10%. Nevertheless, the γ-rays at 277.6 keV were preferred over others in the calculations because the γ-rays at 106.1 keV and 228.2 keV are subjected to interference by the γ-rays at 103.2 keV and 228.2 keV originating from the fission products 153 Sm (T 1/2 = 46.284 h) and 132 Te (T 1/2 = 3.204 d), respectively [4][5][6]. In this experiment, the 197 Au (n, γ)…”
Section: B 238 U Neutron Capture Cross-section Calculationmentioning
confidence: 99%
“…The radionuclide 239 Pu is produced by the 238 U (n, γ) reaction and two consecutive beta decays of 239 U [3,4]. The yield of 239 Pu relies on the 238 U (n, γ) 239 U reaction cross-section, resulting in the requirement to determine the precise reaction cross-sectional values of 238 U (n, γ) 239 U to anticipate the dynamical behaviors of complicated arrangements and security [4,5]. Meanwhile, the value of the conversion ratio, the ratio of the amount of nuclear fuel produced by the fast reactor operation to the consumption, depends on the 238 U neutron capture crosssection.…”
Section: Introductionmentioning
confidence: 99%