Neutron Total Cross Sections of181Ta and238U from 24.3 keV to 1 MeV and Average Resonance Parameters

1984 ◽  
Vol 88 (4) ◽  
pp. 579-591 ◽  
Author(s):  
Izumi Tsubone ◽  
Yutaka Nakajima ◽  
Yutaka Furuta ◽  
Yukinori Kanda
2016 ◽  
Vol 183 (2) ◽  
pp. 286-297 ◽  
Author(s):  
Taofeng Wang ◽  
Guinyun Kim ◽  
Young Do Oh ◽  
Moo-Hyun Cho ◽  
In Soo Ko ◽  
...  

1978 ◽  
Vol 45 (6) ◽  
pp. 1189-1191 ◽  
Author(s):  
V. A. Anufriev ◽  
T. S. Belanova ◽  
Yu. S. Zamyatnin ◽  
A. G. Kolesov ◽  
S. N. Nikol'skii ◽  
...  

2021 ◽  
Author(s):  
Jie Ren ◽  
xichao ruan ◽  
Wei Jiang ◽  
Jie Bao ◽  
jincheng wang ◽  
...  

Abstract The capture cross sections of the 169Tm(n, γ) reaction were measured at the back streaming white neutron beam line (Back-n) of the China Spallation Neutron Source (CSNS) using four C6D6 liquid scintillation detectors. To obtain accurate cross sections, the background subtraction, normalization, and correction were carefully taken into consideration in the data analysis. For the resonance at 3.9 eV, the R-matrix code SAMMY was used to determine the resonance parameters with internally normalization method. While the average capture cross sections of 169Tm in the energy range between 30 keV and 300 keV were extracted relative to the 197Au(n, γ) reaction. The measured cross sections of the 169Tm(n, γ) reaction were reported in logarithmically equidistant energy bins with 20 bins per energy decade with a total uncertainty of 5.4%-7.0% in this paper, and described in terms of average resonance parameters by means of a Hauser-Feshbach calculation with fluctuations. Both of the point-wise cross sections and the averge resonance parameters showed fair agreement with the evaluated values of ENDF/B-VIII.0 library in the energy region studied.


1977 ◽  
Vol 15 (2) ◽  
pp. 600-614 ◽  
Author(s):  
M. S. Pandey ◽  
J. B. Garg ◽  
J. A. Harvey

Pramana ◽  
2007 ◽  
Vol 68 (2) ◽  
pp. 279-287
Author(s):  
A. K. M. Moinul Haque Meaze ◽  
K. Devan ◽  
Y. S. Lee ◽  
Y. D. Oh ◽  
G. N. Kim ◽  
...  

1972 ◽  
Vol 50 (17) ◽  
pp. 1978-1986
Author(s):  
M. D. Ricabarra ◽  
R. Turjanski ◽  
G. H. Ricabarra

Values of the reduced activation resonance integral relative to the thermal cross section I′/σ0 of 74Ge and 76Ge were determined relative to gold by measuring cadmium ratios in a reactor spectrum.A lithium-drifted germanium γ-ray spectrometer was used to resolve the activities of the samples.The results for 74Ge are I′/σ0 = 1.514 ± 0.031 and I′ = 0.681 ± 0.123 b with an assumed σ0 = 0.45 ± 0.08 b; for 76GeI′/σ0 = 12.00 ± 0.16 and I′ = 1.992 ± 0.359 with an assumed σ0 = 0.166 ± 0.030 b.The values obtained for I′ are in serious disagreement with the values calculated with neutron resonance parameters and confirm previous results obtained in similar keV average resonance spacing isotopes.Due to this fact a careful evaluation of the keV neutron radiative capture cross section and resonance integral for 74Ge was undertaken.The evaluation and comparison with the experimental value of the resonance integral shows first that for nuclides with an average resonance spacing of keV the unresolved resonance integral has been seriously underestimated in many evaluations, and second that between 10 and 100 keV, resonance integrals calculated with smooth low resolution activation cross sections give a better calculation of neutron captures than that obtained with neutron resonance parameters.


1987 ◽  
Vol 62 (3) ◽  
pp. 241-242 ◽  
Author(s):  
L. L. Litvinskii ◽  
V. P. Vertebnyi ◽  
V. A. Libman ◽  
A. V. Murzin

1987 ◽  
Vol 42 (9) ◽  
pp. 909-916 ◽  
Author(s):  
K. Knopf ◽  
W. Waschkowski

The coherent neutron scattering lengths and total cross sections of elemental and oxide samples of natural and isotopically enriched W are determined. From these results the following coherent scattering lengths, b, and absorptions at 0.0253 eV, σγ were deduced:b (natW) = 4.86±0.02 fm, σγ = 17.3 ±0.5 b ,b (182W) = 7.04±0.04 fm, σγ = 19.6±0.3 b ,b (183W) = 6.59±0.04 fm, σγ = 10.5±0.2 b ,b (184W) = 7.55±0.06 fm, σγ = 1.7±0.1 b ,b (186W) = -0 .7 3±0.04 fm, σγ = 38.5 ±0.8 b .By comparison with the resonance parameters, the incoherence and the potential radii are derived and discussed. The bound level on W-182 must be fitted with a scattering width of gI0n = 161 meV at E0 = - 94 eV.


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