NEUTRON YIELDS FROM ACTINIDE–BERYLLIUM ALLOYS

1956 ◽  
Vol 34 (9) ◽  
pp. 949-958 ◽  
Author(s):  
O. J. C. Runnalls ◽  
R. R. Boucher

The neutron yields from the reaction Be9(α, n)C12 have been measured for several actinide–beryllium alloys. The values for the beryllium thick target neutron yield, derived from the measurements on alloys containing Pu239, Am241, and Cm242, are 60 ± 2, 74 ± 2, and 112 ± 3 neutrons per million alphas, respectively, when based on the Chalk River standard Ra226-α-Be source. The dependence of the thick target yield, nmax, on the alpha-particle energy, E, is described by the empirical formula nmax = 0.152 E3.65 neutrons per million alphas. The yields for Ra-α-Be and Ac227-α-Be, calculated from the latter expression, are in reasonable agreement with the best observed yields from powder-compacted sources. For Po-α-Be, the calculated thick target yield of 67 neutrons per million alphas lies within the limits of error of the yield observed by several earlier workers.

1987 ◽  
Vol 35 (2) ◽  
pp. 467-478 ◽  
Author(s):  
I. Kumabe ◽  
Y. Mito ◽  
M. Hyakutake ◽  
N. Koori ◽  
H. Sakai ◽  
...  

2014 ◽  
Vol 922 ◽  
pp. 112-125 ◽  
Author(s):  
Gy. Gyürky ◽  
M. Vakulenko ◽  
Zs. Fülöp ◽  
Z. Halász ◽  
G.G. Kiss ◽  
...  

2001 ◽  
Vol 34 (1-6) ◽  
pp. 341-343 ◽  
Author(s):  
C Amero ◽  
J.I Golzarri ◽  
M Izerrouken ◽  
G Espinosa

1951 ◽  
Vol 84 (6) ◽  
pp. 1219-1221 ◽  
Author(s):  
John D. Seagrave

Author(s):  
Hicham Harrass ◽  
Abdellatif Talbi ◽  
Rodouan Touti

Abstract CR-39 and LR-115 type II solid state nuclear track detectors (SSNTDs) are both used, in order to assess the concentration of nucleus belonging to 238U and 232Th series, these ones can be also used to measure radon 222Rn and thoron 220Rn gases in different locations. In this paper, a Monte Carlo code was developed to calculate the mean critical angle for which alpha particles emitted from 238U and 232Th families in studied material samples reach CR-39 and LR-115 type II surfaces and bring about latent tracks on them. The dependence of the SSNTDs mean critical angle on the removed thickness, the initial alpha particle energy has been studied. A linear relationship between CR-39 mean critical angle and the initial alpha particle energy for different removed thicknesses has been found. This straightforward relationship allows determining quickly the mean critical angle of etching which corresponds to initial alpha particle energy for a given removed thickness. CR-39 mean critical angle ranged from 59° for an alpha particle emitted by 212Po to 71° for an alpha particle emitted by 232Th, for the value of removed thickness of 6 µm; whereas LR-115 type II mean critical angle does not depend on the initial alpha particle energy except for 232Th, 238U, 230Th and 234Ra when the removed thickness ranged from 6 µm to 8 µm. Obtained data by using the current method and those obtained in the literature [18] are in good agreement with each other.


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