scholarly journals Alpha-decay Half-lives and Fission Barriers for Superheavy Nuclei Predicted by a Nuclear Mass Formula

2002 ◽  
Vol 3 (1) ◽  
pp. 201-203 ◽  
Author(s):  
H. Koura
2004 ◽  
Vol 13 (01) ◽  
pp. 79-86 ◽  
Author(s):  
J. F. BERGER ◽  
D. HIRATA ◽  
M. GIROD ◽  
J. DECHARGE

This contribution summarizes the predictions obtained in the domain of superheavy nuclei from self-consistent microscopic calculations employing the Gogny force. Results concerning shell gaps, fission barriers and stability against alpha-decay are recalled. Recent work involving α-decay chains in odd nuclides is also presented and discussed.


2002 ◽  
Vol 39 (sup2) ◽  
pp. 774-777 ◽  
Author(s):  
Hiroyuki Koura ◽  
Takahiro Tachibana ◽  
Tadashi Yoshida

2016 ◽  
Vol 951 ◽  
pp. 60-74 ◽  
Author(s):  
A.I. Budaca ◽  
R. Budaca ◽  
I. Silisteanu

2018 ◽  
Author(s):  
U. K. Singh ◽  
M. Kumawat ◽  
G. Saxena ◽  
M. Kaushik ◽  
S. K. Jain

2018 ◽  
Vol 27 (02) ◽  
pp. 1850015 ◽  
Author(s):  
S. Cht. Mavrodiev ◽  
M. A. Deliyergiyev

We formalized the nuclear mass problem in the inverse problem framework. This approach allows us to infer the underlying model parameters from experimental observation, rather than to predict the observations from the model parameters. The inverse problem was formulated for the numerically generalized semi-empirical mass formula of Bethe and von Weizsäcker. It was solved in a step-by-step way based on the AME2012 nuclear database. The established parametrization describes the measured nuclear masses of 2564 isotopes with a maximum deviation less than 2.6[Formula: see text]MeV, starting from the number of protons and number of neutrons equal to 1.The explicit form of unknown functions in the generalized mass formula was discovered in a step-by-step way using the modified least [Formula: see text] procedure, that realized in the algorithms which were developed by Lubomir Aleksandrov to solve the nonlinear systems of equations via the Gauss–Newton method, lets us to choose the better one between two functions with same [Formula: see text]. In the obtained generalized model, the corrections to the binding energy depend on nine proton (2, 8, 14, 20, 28, 50, 82, 108, 124) and ten neutron (2, 8, 14, 20, 28, 50, 82, 124, 152, 202) magic numbers as well on the asymptotic boundaries of their influence. The obtained results were compared with the predictions of other models.


Author(s):  
J. M. Pearson ◽  
F. Tondeur ◽  
A. K. Dutta
Keyword(s):  

2003 ◽  
pp. 15-18
Author(s):  
J. M. Pearson ◽  
S. Goriely ◽  
M. Samyn

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