scholarly journals Fission of super-heavy nuclei: Fragment mass distributions and their dependence on excitation energy

2019 ◽  
Vol 3 (1) ◽  
pp. 10-17
Author(s):  
N. Carjan ◽  
F.A. Ivanyuk ◽  
Yu.Ts. Oganessian
2015 ◽  
Vol 748 ◽  
pp. 89-94 ◽  
Author(s):  
K. Nishio ◽  
A.N. Andreyev ◽  
R. Chapman ◽  
X. Derkx ◽  
Ch.E. Düllmann ◽  
...  

Open Physics ◽  
2014 ◽  
Vol 12 (8) ◽  
Author(s):  
Subrata Biswal ◽  
Suresh Patra

AbstractWe study the isoscalar giant monopole resonance for drip-lines and super heavy nuclei in the framework of relativistic mean field theory with a scaling approach. The well known extended Thomas-Fermi approximation in the nonlinear σ-ω model is used to estimate the giant monopole excitation energy for some selected light spherical nuclei starting from the region of proton to neutron drip-lines. The application is extended to the super heavy region for Z=114 and 120, which are predicted by several models as the next proton magic numbers beyond Z=82. We compared the excitation energy obtained by four successful force parameters NL1, NL3, NL3*, and FSUGold. The monopole energy decreases toward the proton and neutron drip-lines in an isotopic chain for lighter mass nuclei, in contrast to a monotonic decrease for super heavy isotopes. The maximum and minimum monopole excitation energies are obtained for nuclei with minimum and maximum isospin in an isotopic chain, respectively.


2011 ◽  
Vol 312 (8) ◽  
pp. 082010
Author(s):  
E Andrade-II ◽  
J C M Menezes ◽  
S B Duarte ◽  
F Garcia ◽  
P C R Rossi ◽  
...  

2011 ◽  
Vol 38 (8) ◽  
pp. 085104 ◽  
Author(s):  
E Andrade-II ◽  
J C M Menezes ◽  
S B Duarte ◽  
F Garcia ◽  
P C R Rossi ◽  
...  

2015 ◽  
Vol 92 (2) ◽  
Author(s):  
R. Tripathi ◽  
S. Sodaye ◽  
K. Sudarshan ◽  
B. K. Nayak ◽  
A. Jhingan ◽  
...  

Nuclear disintegrations produced in the heavy nuclei of Ilford G 5 photographic emulsions by 950 MeV protons have been analyzed in detail. The characteristics of the disintegrations observed can be explained in terms of a simple model which assumes that a substantial fraction of the π mesons created is reabsorbed in the parent nucleus and that the energy of these mesons contributes mainly to the excitation energy of the residual nucleus.


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