Fully microscopic scission-point model to predict fission fragment observables

2019 ◽  
Vol 99 (3) ◽  
Author(s):  
J.-F. Lemaître ◽  
S. Goriely ◽  
S. Hilaire ◽  
J.-L. Sida
2014 ◽  
Vol 69 ◽  
pp. 00016
Author(s):  
Stefano Panebianco ◽  
Nöel Dubray ◽  
Stéphane Goriely ◽  
Stéphane Hilaire ◽  
Jean-François Lemaître ◽  
...  

2015 ◽  
Vol 92 (3) ◽  
Author(s):  
Jean-François Lemaître ◽  
Stefano Panebianco ◽  
Jean-Luc Sida ◽  
Stéphane Hilaire ◽  
Sophie Heinrich

2018 ◽  
Vol 27 (03) ◽  
pp. 1850018 ◽  
Author(s):  
M. R. Pahlavani ◽  
P. Mehdipour

Photofission of [Formula: see text]Th, [Formula: see text]U, [Formula: see text]Np and [Formula: see text]Pu isotopes are investigated. Modified version of Gorodisskiy approach that is developed to study the neutron-induced fission are employed to simulate fission fragment mass distribution for these isotopes in different energies. The effect of emitted neutron prior to scission point is studied. Peak to valley ratio is also extracted. Obtained results using this approach are compared with original Gorodisskiy model as well as available experimental data. Satisfactory agreement is achieved between theoretical and experimental data especially in medium and low [Formula: see text]-ray energies than original formalism of Gorodisskiy.


Author(s):  
V. A. KALININ ◽  
V. N. DUSHIN ◽  
B. F. PETROV ◽  
V. A. JAKOVLEV ◽  
A. S. VOROBYEV ◽  
...  

2021 ◽  
Vol 9 ◽  
Author(s):  
P. Mehdipour Kadiani

The photofission fragment mass yields of actinides are evaluated using a systematic statistical scission point model. In this model, all energies at the scission point are presented as a linear function of the mass numbers of fission fragments. The mass yields are calculated with a new approximated relative probability for each complementary fragment. The agreement with the experimental data is quite good, especially with a collective temperature Tcol of 2 MeV at intermediate excitation energy and Tcol = 1 MeV for spontaneous fission. This indicates that the collective temperature is greater than the value obtained by the initial excitation energy. The generalized superfluid model is applied for calculating the fragment temperature. The deformation parameters of fission fragments have been obtained by fitting the calculated results with the experimental values. This indicates that the deformation parameters decrease with increasing excitation energy. Also, these parameters decrease for fissioning systems with odd mass numbers.


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