Fragment Mass Distributions for Thermal-Neutron-Induced Fission ofPu239andPu241

1964 ◽  
Vol 133 (6B) ◽  
pp. B1500-B1502 ◽  
Author(s):  
F. J. Walter ◽  
H. W. Schmitt ◽  
J. H. Neiler
2011 ◽  
Vol 83 (5) ◽  
Author(s):  
I. V. Ryzhov ◽  
S. G. Yavshits ◽  
G. A. Tutin ◽  
N. V. Kovalev ◽  
A. V. Saulski ◽  
...  

1975 ◽  
Vol 11 (5) ◽  
pp. 1676-1680 ◽  
Author(s):  
K. F. Flynn ◽  
J. E. Gindler ◽  
R. K. Sjoblom ◽  
L. E. Glendenin

1987 ◽  
Vol 42 (8) ◽  
pp. 786-790 ◽  
Author(s):  
H.-H. Knitter ◽  
F.-J. Hambsch ◽  
C. Budtz-Jørgensen ◽  
J. P. Theobald

A formula for the fission fragment yield area in the coordinate system of the fragment total kinetic energy and of the fragment mass is presented. It was deduced along the lines of the multiexit- channel model of fission elaborated by Brosa, Grossmann and Müller. This formula was fitted to the fragment mass-, average total kinetic energy-, and variance distributions of the thermal neutron induced fission of 235U. The obtained parameters are compared with the theoretical predictions. Further improvements of the fragment yield representation are discussed.


2009 ◽  
Author(s):  
V. D. Simutkin ◽  
I. V. Ryzhov ◽  
G. A. Tutin ◽  
L. A. Vaishnene ◽  
J. Blomgren ◽  
...  

2021 ◽  
Vol 68 (1 Jan-Feb) ◽  
Author(s):  
Modesto Montoya ◽  
Oliver Páucar ◽  
A. Obregón ◽  
A. Aponte

Using a Monte Carlo method, we simulate the measurement, by the 2E technique, of the average prompt neutron multiplicity as a function of the mass of fragments from the thermal neutron-induced fission of 239Pu. The input data for the simulation, associated with the primary fragment mass (A), consist of the yield (Y), the distribution of the total kinetic energy characterized by its average ((TKE) ̅) and its standard deviation (σ_TKE), the average prompt neutron multiplicity (ν ̅_s, a sawtooth approach of experimental data), and the slope of neutron multiplicity against total kinetic energy (dν_s/d<TKE>). The output data, associated with the simulated as the fragment mass measured by the 2E technique (µ), consist of the yield (y), the distribution of the total kinetic energy characterized by its average ((tke) ̅) and its standard deviation (σ_tke), and the average prompt neutron multiplicity (ν ̅_µ). In the mass regions A≈115 and A>150, ν ̅_µ is higher than ν ̅_s. This result suggests that, in those mass regions, the 2E experimental values associated with the average neutron multiplicity are overestimated, referred to the corresponding to the primary fragments.


1983 ◽  
Vol 27 (3) ◽  
pp. 1117-1125 ◽  
Author(s):  
H. Thierens ◽  
A. De Clercq ◽  
E. Jacobs ◽  
M. Piessens ◽  
P. D'hondt ◽  
...  

Sign in / Sign up

Export Citation Format

Share Document