2018
DOI: 10.1103/physrevc.97.044621
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α decay and cluster radioactivity of nuclei of interest to the synthesis of Z=119 , 120 isotopes

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Cited by 57 publications
(30 citation statements)
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“…This phenomenon, first observed in 1984 (Rose and Jones, 1984) as the emission of 14 C from 223 Ra, has since been confirmed in a number of heavy nuclei with Z > 86, which decay by emitting light clusters between 14 C and 34 Si, as well as in superheavy nuclei with Z ≤ 116 (Itkis et al, 2015;Kozulin et al, 2014). For superheavy nuclei with Z ≥ 118, cluster radioactivity is expected to become competitive with alpha decay and spontaneous fission (Poenaru and Gherghescu, 2018;Poenaru et al, 2011Poenaru et al, , 2012Poenaru et al, , 2013Poenaru et al, , 2015Santhosh and Nithya, 2018a;Zhang and Wang, 2018). Microscopically, cluster emission can be considered as an extremely asymmetric fission, with the heavy fragment corresponding to a nucleus in the neighborhood of the doubly-magic 208 Pb (Warda and Robledo, 2011).…”
Section: Fissionmentioning
confidence: 75%
“…This phenomenon, first observed in 1984 (Rose and Jones, 1984) as the emission of 14 C from 223 Ra, has since been confirmed in a number of heavy nuclei with Z > 86, which decay by emitting light clusters between 14 C and 34 Si, as well as in superheavy nuclei with Z ≤ 116 (Itkis et al, 2015;Kozulin et al, 2014). For superheavy nuclei with Z ≥ 118, cluster radioactivity is expected to become competitive with alpha decay and spontaneous fission (Poenaru and Gherghescu, 2018;Poenaru et al, 2011Poenaru et al, , 2012Poenaru et al, , 2013Poenaru et al, , 2015Santhosh and Nithya, 2018a;Zhang and Wang, 2018). Microscopically, cluster emission can be considered as an extremely asymmetric fission, with the heavy fragment corresponding to a nucleus in the neighborhood of the doubly-magic 208 Pb (Warda and Robledo, 2011).…”
Section: Fissionmentioning
confidence: 75%
“…for even-even, even-odd, odd-even and odd-odd isotopes, respectively. The models mentioned above strongly depend on the even-odd property of the number of proton Z and neutron N. Since the heavy nuclei often have a strong deformation which is dependent on the asymmetry of the nuclei, D. N. Poenaru [11][12][13] proposed a new model based on the Royer formula by adding two factors in terms of the asymmetric factor, I = (N-Z)/A. The new formula reads Notice here that Poenaru model in Equation (3) is dependent on the asymmetry of the nuclei and the evenodd property has been removed.…”
Section: Theoretical Frameworkmentioning
confidence: 99%
“…In this work, we estimate the half-life to deduce the critical concentrations of the isotopes in the samples corresponding to the limit of the analysis. The α-decay half-lives are re-examined via few methods such as the semi-empirical formulae of the Viola-Seaborg relationship 10 , the Poenaru method [11][12][13] , and the Royer approach 14,15 which have been improved to increase the accuracy of the half-life prediction. The uncertainties of the half-lives, decay constants and the radioactivity of the exotic nuclei in the 232 Th decay chain are also investigated.…”
mentioning
confidence: 99%
“…The following types of radioactivities have been experimentally confirmed worldwide (Oxford, Moscow, Orsay, Berkeley, Geneva, Dubna, Argonne, Milano, Viena, Lanzhou, Beijing and Livermore) [26]: 14 C, 20 O, 23 F, 22 , [24][25][26] Ne, 28,30 Mg and 32,34 Si from parent nuclides with Z = 87 -96. There are about 26 different successful experiments.…”
Section: Introductionmentioning
confidence: 99%