论文标题

核四极变形和电荷半径的统计相关性

Statistical correlations of nuclear quadrupole deformations and charge radii

论文作者

Reinhard, Paul-Gerhard, Nazarewicz, Witek

论文摘要

形状变形和电荷半径,原子核的基本特性,都受核力量的全局特征和核子壳结构的影响。作为质子和中子数的功能,两个量都显示出规则的模式,对于远离魔术数的核,它们从核从核变为核的变化非常顺利。在本文中,我们解释了局部壳的效应如何影响四极变形与均匀成型的均匀,YB和HF同位素的统计相关性。这反过来意味着,相关性突然变化可能是壳效应的有用指标。我们的理论分析是在使用量化的能量密度函数和密度依赖性配对力的均匀平均场理论框架内进行的。统计分析是通过线性最小二乘回归进行的。核四极变形和电荷半径的局部变化,用职业来解释,个人变形的Hartree-fock轨道,对计算可观察到的统计相关性的创造和烙印。在某些情况下,计算出的变形或电荷半径与其甚至邻居的半径相关,但相关性似乎随粒子数而迅速恶化。核变形与不同核的电荷半径之间的统计相关性受到基础壳结构的影响。即使对于这些可观察到的核变形良好和超氟的核,相关范围通常不超过$Δn= 4 $和$Δz= 4 $,即相当短。该结果表明,通常不能证明平稳变化的可观察到的统计误差的假设通常是合理的。

Shape deformations and charge radii, basic properties of atomic nuclei, are influenced by both the global features of the nuclear force and the nucleonic shell structure. As functions of proton and neutron number, both quantities show regular patterns and, for nuclei away from magic numbers, they change very smoothly from nucleus to nucleus. In this paper, we explain how the local shell effects are impacting the statistical correlations between quadrupole deformations and charge radii in well-deformed even-even Er, Yb, and Hf isotopes. This implies, in turn, that sudden changes in correlations can be useful indicators of underlying shell effects. Our theoretical analysis is performed in the framework of self-consistent mean-field theory using quantified energy density functionals and density-dependent pairing forces. The statistical analysis is carried out by means of the linear least-square regression. The local variations of nuclear quadrupole deformations and charge radii, explained in terms of occupations individual deformed Hartree-Fock orbits, make and imprint on statistical correlations of computed observables. While the calculated deformations or charge radii are, in some cases, correlated with those of their even-even neighbors, the correlations seem to deteriorate rapidly with particle number. The statistical correlations between nuclear deformations and charge radii of different nuclei are affected by the underlying shell structure. Even for well deformed and superfluid nuclei for which these observables change smoothly, the correlation range usually does not exceed $ΔN=4$ and $ΔZ=4$, i.e., it is rather short. This result suggests that the frequently made assumption of reduced statistical errors for the differences between smoothly-varying observables cannot be generally justified.

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