The kinks in charge radii across N = 82 and 126 revisited

M. Bhuyan, B. Maheshwari, H. A. Kassim, N. Yusof, S. Patra, B. V. Carlson, P. Stevenson
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引用次数: 3

Abstract

We revisit the studies of the isotopic shift in the charge radii of {\it even-even} isotopes of Sn and Pb nuclei at $N$ = 82, and 126, respectively, within the relativistic mean-field and Relativistic-Hartree-Bogoliubov approach. The shell model is also used to estimate isotopic shift in these nuclei, for the first time, to the best of our knowledge. The ground state single-particle energies ($spe$) are calculated for non-linear NL3 \& NL3$^*$ and density-dependent DD-ME2 parameter sets compared with the experimental data, wherever available. We establish a correlation between the filling of single-particle levels and the isotopic shift in occupation probabilities. The obtained $spe$ from the relativistic mean-field and Relativistic-Hartree-Bogoliubov approaches are in line with those used in the shell model and experimental data for both the Sn and Pb isotopic chains. The shell model calculated isotopic shift agrees with relativistic mean-field and Relativistic-Hartree-Bogoliubov approaches that explain the experimental data quite well.
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重新考察了N = 82和126之间的电荷半径
本文在相对论平均场和相对论hartree - bogoliubov方法下,重新研究了Sn和Pb原子核在N = 82和126处的偶偶同位素电荷半径的同位素位移。据我们所知,壳层模型还首次用于估计这些原子核中的同位素位移。计算了非线性NL3 \& NL3$^*$和密度相关的DD-ME2参数集的基态单粒子能量($spe$),并与实验数据进行了比较。我们建立了单粒子能级的填充与占据概率的同位素位移之间的关系。从相对论平均场和相对论hartree - bogoliubov方法得到的$spe$与Sn和Pb同位素链的壳模型和实验数据一致。壳模型计算的同位素位移与相对论平均场和相对论- hartree - bogoliubov方法一致,这两种方法都能很好地解释实验数据。
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