Ranges of shielded nuclides from thermal-neutron fission

1969 ◽  
Vol 47 (21) ◽  
pp. 2371-2385 ◽  
Author(s):  
H. Nakahara ◽  
J. W. Harvey ◽  
G. E. Gordon

Average ranges in Al of shielded nuclides 86Rb and 136Cs and several chain-yield species from thermal-neutron fission of 233U and 235U have been measured. The values obtained (in mg/cm2 Al) are, for 233U: 86Rb, 3.88 ± 0.04; 136CS, 2.80 ± 0.01; and for 235U: 86Rb, 3.76 ± 0.03; 136Cs, 2.81 ± 0.01. A range–energy transformation was used to determine average kinetic energies [Formula: see text] of the secondary fragments. In agreement with previous work, the shielded nuclides are found to have smaller [Formula: see text] values than neighboring chain-yield species. The deficits of [Formula: see text] are, for 233U, 4 and 8 MeV, and for 235U, 8 and 10 MeV, respectively, for 86Rb and 136Cs. Most of the range experiments were done with the thick-catcher method followed by conventional radiochemical treatment of the catcher foils. Ranges of 20 products from 233U were determined in preliminary experiments in which gross γ-ray spectra of fission products in the catcher foils were observed with a Ge(Li) detector. The kinetic-energy deficits of the shielded species are interpreted by Monte Carlo calculations of prompt-neutron emission.

1970 ◽  
Vol 48 (14) ◽  
pp. 1708-1715 ◽  
Author(s):  
B. L. Tracy ◽  
H. G. Thode

Absolute independent yields of the shielded nuclides 80Br, 82Br, 128I, and 130I produced in the thermal neutron fission of 235U, 239Pu, and 233U have been determined by careful mass spectrometric analyses of krypton and xenon fission products. In addition, a fractional independent yield of 130I from the thermal neutron fission of 238Np has been determined, and an upper limit has been set for the independent yield of 126I from 235U fission. All the yields from 235U fission except that of 128I are consistent with the Gaussian charge distribution described by Wahl. However, conventional theories of charge distribution in fission do not account for the irregular variation in iodine yields from one fissile nuclide to another. A mechanism based on differences in neutron emission probabilities from prompt fission fragments is proposed in order to explain this variation.


1969 ◽  
Vol 139 (2) ◽  
pp. 289-307 ◽  
Author(s):  
K. Sistemich ◽  
P. Armbruster ◽  
J. Eidens ◽  
E. Roeckl

2014 ◽  
Vol 57 (1) ◽  
pp. 22-27 ◽  
Author(s):  
K. A. Balygin ◽  
M. D. Karetnikov ◽  
A. I. Klimov ◽  
V. I. Kopeikin ◽  
V. A. Kurkin ◽  
...  

1983 ◽  
Vol 61 (4) ◽  
pp. 649-651 ◽  
Author(s):  
L. Toppare ◽  
H. N. Erten ◽  
N. K. Aras

Yields of products both in the light and heavy sides in the spontaneous fission of 252Cf were measured by direct γ-ray spectroscopy technique. By suitably choosing collection, cooling, and counting times, it was possible to observe products with half-lives between 1 min and 1 h. A definite fine structure, as observed in the case of thermal neutron fission of 235U and 239Pu, was not observed. A graphical method was utilized to obtain the number of neutrons as a function of fragment mass using cumulative chain yields.


1989 ◽  
Vol 218 (3) ◽  
pp. 365-368 ◽  
Author(s):  
A.A. Hahn ◽  
K. Schreckenbach ◽  
W. Gelletly ◽  
F. von Feilitzsch ◽  
G. Colvin ◽  
...  

1985 ◽  
Vol 160 (4-5) ◽  
pp. 325-330 ◽  
Author(s):  
K. Schreckenbach ◽  
G. Colvin ◽  
W. Gelletly ◽  
F. Von Feilitzsch

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