Gamma-ray spectrometric measurements of the capture cross section of gold-198 for reactor neutrons

1969 ◽  
Vol 31 (5) ◽  
pp. 1229-1240 ◽  
Author(s):  
M.J. Cabell ◽  
M. Wilkins
2005 ◽  
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Author(s):  
A. Trkov ◽  
G. L. Molnár ◽  
Zs. Révay ◽  
S. F. Mughabghab ◽  
R. B. Firestone ◽  
...  

2011 ◽  
Vol 59 (2(3)) ◽  
pp. 1844-1847 ◽  
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T. Katabuchi ◽  
N. C. Hai ◽  
M. Igashira ◽  
S. Kamada ◽  
M. Tajika ◽  
...  

2016 ◽  
Vol 122 ◽  
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Tatsuya Katabuchi ◽  
Tohomohiro Okamiya ◽  
Shotaro Yanagida ◽  
Motoharu Mizumoto ◽  
Kazushi Terada ◽  
...  

2014 ◽  
Vol 24 (3S2) ◽  
pp. 29-37
Author(s):  
Nguyen Van Do ◽  
Pham Duc Khue ◽  
Kim Tien Thanh ◽  
Nguyen Thi Hien ◽  
Kim Guinyun

Thermal neutron capture cross section and resonance integral for the $^{45}$Sc(n,$\gamma )^{46}$Sc reaction were measured by the activation method using the $^{197}$Au(n,$\gamma )^{198}$Au reaction as a single comparator. The high-purity scandium and gold samples with and without Cd cover with the thickness of 0.5 mm were irradiated in a pulsed neutron field of the 100 MeV electron linac of the Pohang Accelerator Laboratory (PAL). The induced activities in the activated foils were measured with a well calibrated HPGe detector. In order to improve the accuracy of the experimental results the effect of the non-ideal epithermal spectrum was taken in to account by determining the neutron spectrum shape factor ($\alpha )$, and the corrections for the thermal (G$_{th})$ and the resonance (G$_{epi})$ neutron self-shielding effects, the $\gamma $-ray attenuation (F$_{g})$ and the $\gamma $-ray coincidence summing effect were made. The thermal neutron cross-section for the $^{45}$Sc(n,$\gamma )^{46}$Sc reaction has been determined to be $\sigma _{o}$ = 27.6 $\pm $ 0.8 barn. By assuming the cadmium cut-off energy of 0.55 eV, the resonance integral for the $^{45}$Sc(n,$\gamma )^{46}$Sc reaction has been determined to be I$_{o}$ = 12.7 $\pm $ 0.7 bar. The present results are compared with the reference data and discussed.


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