2021
DOI: 10.1016/j.nuclphysa.2020.122066
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Structural properties and α-decay chains of transfermium nuclei (101≤Z≤110)

Abstract: Transfermium nuclei (101≤Z≤110) are investigated thoroughly to describe structural properties viz. deformation, radii, shapes, magicity, etc. as well as their probable decay chains. These properties are explored using relativistic mean-field (RMF) approach and compared with other theories along with available experimental data. Neutron numbers N=152 and 162 have come forth with a deformed shell gap whereas N=184 is ensured as a spherical magic number. The region with N>168 bears witness of the phenomenon of sh… Show more

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Cited by 12 publications
(11 citation statements)
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“…(experimental limit of half-lives of cluster emissions). For examples, 21 Na from 226−229 Np, 22 Na from 226−230 Np, 23 Na from 226−233 Np, 24 Na from 226−234 Np, 25,27 Na from 226−237 Np, 26 Na from 226−236 Np and 28 Na from 224−236 Np. Similarly, some possible clusters (Mg-isotopes) emitted from various Pu-isotopes (Z p =94) are 23 Mg from 226−231 Pu, 24,25 Mg from 226−235 Np, 26 Mg from 226−238 Np, 27 Mg from 226−239 Np, and 28,29 Mg from 226−241 Np.…”
Section: Parent Daughter Emittedmentioning
confidence: 99%
See 1 more Smart Citation
“…(experimental limit of half-lives of cluster emissions). For examples, 21 Na from 226−229 Np, 22 Na from 226−230 Np, 23 Na from 226−233 Np, 24 Na from 226−234 Np, 25,27 Na from 226−237 Np, 26 Na from 226−236 Np and 28 Na from 224−236 Np. Similarly, some possible clusters (Mg-isotopes) emitted from various Pu-isotopes (Z p =94) are 23 Mg from 226−231 Pu, 24,25 Mg from 226−235 Np, 26 Mg from 226−238 Np, 27 Mg from 226−239 Np, and 28,29 Mg from 226−241 Np.…”
Section: Parent Daughter Emittedmentioning
confidence: 99%
“…The importance of angular momentum on the α-decay half-lives has already been established in a few of our recent works [19,20] which has invoked us to probe similar dependence on the cluster decay half-lives. In addition to this, isospin (I = (N − Z)/A) of parent nucleus is found to be pivotal for the case of α-decay in heavy and superheavy nuclei [20][21][22][23][24][25] pointing towards its significance in terms of cluster decay as well. Considering these two effects together, modified UDL formula (new UDL) by Soylu and Qi [26], and improved NRDX formula (named as improved unified formula (IUF)) by Ismail et al [27] have explained recently that angular momentum and isospin are indeed crucial quantities in determining the cluster decay half-lives.…”
Section: Introductionmentioning
confidence: 98%
“…Q α -values required for these calculations are obtained using expression (16). Modified Manjunatha formula (MMF) [66]:…”
Section: Barrier Penetration and Half-lifementioning
confidence: 99%
“…Few of the above-mentioned formulas are refitted using the latest experimental alpha decay half-lives, namely (i) modified Royer GLDM (Rm), modified Viola-Seaborg (VSm1 and VSm2) and modified Sobiczewski-Parkhomenko (SPm1 and SPm2) formulas [41], (ii) a modified version of the Brown empirical formula (mB1 and mB2) [42] (iii) new universal decay law (NUDL), new Royer (NRo) and new Sobiczewski-Parkhomenko (NSP) formulas [43]. Moreover, Manjunatha et al have presented a formula [44] based on secondorder polynomial fitting of Z 0.4 d / √ Q which is subsequently modified in one of our recent works [45].…”
Section: Introductionmentioning
confidence: 99%