scholarly journals α decay properties of 297 Og within the two-potential approach

2017 ◽  
Vol 41 (12) ◽  
pp. 124109 ◽  
Author(s):  
Jun-Gang Deng ◽  
Jun-Hao Cheng ◽  
Bo Zheng ◽  
Xiao-Hua Li
2019 ◽  
Vol 71 (11) ◽  
pp. 1328 ◽  
Author(s):  
Jun-Yao Xu ◽  
Jiu-Long Chen ◽  
Jun-Gang Deng ◽  
Jun-Hao Cheng ◽  
Hong-Ming Liu ◽  
...  

2018 ◽  
Vol 42 (4) ◽  
pp. 044102 ◽  
Author(s):  
Jun-Gang Deng ◽  
Jie-Cheng Zhao ◽  
Jiu-Long Chen ◽  
Xi-Jun Wu ◽  
Xiao-Hua Li

2018 ◽  
Vol 42 (9) ◽  
pp. 094101
Author(s):  
Jing Zhang ◽  
E De-Jun ◽  
Hong-Fei Zhang

2020 ◽  
Vol 44 (10) ◽  
pp. 104102
Author(s):  
Zhishuai Ge ◽  
Gen Zhang ◽  
Shihui Cheng ◽  
Yu. S. Tsyganov ◽  
Feng-Shou Zhang
Keyword(s):  
Α Decay ◽  

2019 ◽  
Vol 100 (5) ◽  
Author(s):  
L. Ghys ◽  
A. N. Andreyev ◽  
M. Huyse ◽  
P. Van Duppen ◽  
S. Antalic ◽  
...  
Keyword(s):  
Α Decay ◽  

2007 ◽  
Vol 16 (04) ◽  
pp. 949-956 ◽  
Author(s):  
YURI OGANESSIAN

The formation and decay properties of the heaviest nuclei with Z = 112 - 116 and 118 were studied in the reactions 238 U , 242,244 Pu , 243 Am , 245,248 Cm and 249 Cf +48 Ca . The new nuclides mainly undergo sequential α-decay, which ends with spontaneous fission. The total time of decays ranges from 0.5 ms to about 1 day, depending on the proton and neutron numbers in the synthesized nuclei. The atomic number of the new elements 115 and 113 was confirmed also by an independent radiochemical experiment based on the identification of the neutron-rich isotope 268 Db (TSF ≈ 30 h ), the final product in the chain of α-decays of the odd–odd parent nucleus 288115. The comparison of the decay properties of 29 new nuclides with Z = 104 - 118 and N = 162 - 177 gives evidence for the decisive influence of the structure of superheavy nuclei on their stability with respect to different modes of radioactive decay. The investigations connected with the search for superheavy elements in Nature (cosmic rays) and prospects of superheavy element research are also presented.


1996 ◽  
Vol 53 (5) ◽  
pp. 2513-2515 ◽  
Author(s):  
K. S. Toth ◽  
J. C. Batchelder ◽  
C. R. Bingham ◽  
L. F. Conticchio ◽  
W. B. Walters ◽  
...  
Keyword(s):  
Α Decay ◽  

2015 ◽  
Vol 24 (04) ◽  
pp. 1550028 ◽  
Author(s):  
M. Bhuyan ◽  
S. Mahapatro ◽  
S. K. Singh ◽  
S. K. Patra

We study the bulk properties such as binding energy (BE), root-mean-square (RMS) charge radius, quadrupole deformation etc. for Francium (Fr) isotopes having mass number A = 180–240 within the framework of relativistic mean field (RMF) theory. Systematic comparisons are made between the calculated results from RMF theory, Finite Range Droplet Model (FRDM) and the experimental data. Most of the nuclei in the isotopic chain shows prolate configuration in their ground state. The α-decay properties like α-decay energy and the decay half-life are also estimated for three different chains of 198 Fr , 199 Fr and 200 Fr . The calculation for the decay half-life are carried out by taking two different empirical formulae and the results are compared with the experimental data.


2019 ◽  
Vol 28 (10) ◽  
pp. 1950089 ◽  
Author(s):  
Hong-Ming Liu ◽  
Jun-Yao Xu ◽  
Jun-Gang Deng ◽  
Biao He ◽  
Xiao-Hua Li

In this work, we systematically study the [Formula: see text] decay half-lives of 170 even–even nuclei with [Formula: see text] within the two-potential approach while the [Formula: see text] decay preformation factor [Formula: see text] is obtained by the cluster-formation model. The calculated results can well reproduce the experimental data. In addition, we extend this model to predict the [Formula: see text] decay half-lives of 64 even–even nuclei with [Formula: see text] whose [Formula: see text] decay is energetically allowed or observed but not yet quantified. For comparison, the two famous models i.e., SemFIS proposed by Poenaru et al. [Europhys. Lett. 77 (2007) 62001] and UDL proposed by Qi et al. [Phys. Rev. Lett. 103 (2009) 072501] are used. The predicted results of these models are basically consistent. At the same time, through analyzing the changing trend of [Formula: see text] decay energy [Formula: see text] of [Formula: see text] and 128 isotopes nuclei with the increasing of neutron number N and that of [Formula: see text] decay preformation factor [Formula: see text] of those isotopes even–even nuclei with the increasing of neutron number N, [Formula: see text] may be a new neutron magic number.


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