236U radiative neutron capture cross section for En=0.3?2.2 MeV

1988 ◽  
Vol 64 (2) ◽  
pp. 179-181 ◽  
Author(s):  
Yu. N. Trofimov
2017 ◽  
Vol 96 (2) ◽  
Author(s):  
B. Baramsai ◽  
M. Jandel ◽  
T. A. Bredeweg ◽  
E. M. Bond ◽  
A. R. Roman ◽  
...  

2018 ◽  
Vol 178 ◽  
pp. 04001
Author(s):  
Stephane Goriely ◽  
Stephane Hilaire ◽  
Sophie Péru

Valuable theoretical predictions of nuclear dipole excitations in the whole chart are of great interest for different nuclear applications, including in particular nuclear astrophysics. Here we extend our large-scale calculations of the E1 and M1 absorption γ-ray strength function obtained in the framework of the axially-symmetric deformed quasiparticle random phase approximation (QRPA) based on the finite-range D1M Gogny force to the determination of the de-excitation strength function. To do so, shell-model calculations of the de-excitation dipole strength function as well as experimental data are considered to provide insight in the low-energy limit and to complement the QRPA estimate phenomenologically. We compare our final prediction of the E1 and M1 strengths with available experimental data at low energies and show that a relatively good agreement can be obtained. Its impact on the average radiative width as well as radiative neutron capture cross section is discussed.


2007 ◽  
Vol 76 (4) ◽  
Author(s):  
C. Domingo-Pardo ◽  
U. Abbondanno ◽  
G. Aerts ◽  
H. Álvarez ◽  
F. Alvarez-Velarde ◽  
...  

2020 ◽  
Vol 239 ◽  
pp. 17021
Author(s):  
Jie Ren ◽  
Xichao Ruan ◽  
Jie Bao ◽  
Guangyuan Luan ◽  
Hanxiong Huang ◽  
...  

Radiative neutron capture cross sections are very important in the field of basic physics research and nuclear device R&D. The Back-n white neutron beam line of China Spallation Neutron Source (CSNS) is the first spallation neutron beam line in China. On the purpose for radiative neutron capture cross section measurement, a C6D6 detector system was built in the Back-n experimental station. The pulse height weighting technique (PHWT) was used to make the system’s detective efficiency independent of the cascade path and the energy of cascade gamma rays. The neutron energy spectrum was measured for the energy between 1eV and 80keV with a 6Li loaded ZnS scintillation detector. Besides, a testing experiment with 197Au and 169Tm samples was carried out to examine this system. According to the preliminary results, this C6D6 detector system can be used to perform neutron capture cross section measurement.


Author(s):  
Yu Kodama ◽  
Tatsuya Katabuchi ◽  
Gerard Rovira ◽  
Atsushi Kimura ◽  
Shoji Nakamura ◽  
...  

1953 ◽  
Vol 31 (3) ◽  
pp. 204-206 ◽  
Author(s):  
Rosalie M. Bartholomew ◽  
R. C. Hawkings ◽  
W. F. Merritt ◽  
L. Yaffe

The thermal neutron capture cross sections of Na23 and Mn55 have been determined using the activation method. The values are 0.53 ± 0.03 and 12.7 ± 0.3 barns respectively with respect to σAul97 = 93 barns. These agree well with recent pile oscillator results. The half-life for Mn56 is found to be 2.576 ± 0.002 hr.


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