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arXiv 2004.04378nucl-th
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Gogny能量密度泛函参数化D1M $^{*}$对超重核fission的微观描述

Microscopic description of fission in superheavy nuclei with the parametrization D1M$^{*}$ of the Gogny energy density functional

R. Rodríguez-Guzmán, Y. M. Humadi, L. M. Robledo

摘要:

基于Gogny能量密度泛函的最新参数化D1 M $^{*}$,用约束Hartree-Fock-Bogoliubov近似描述了435个超重核的裂变. Gogny-D1 M $^{*}$参数化是对现有的实验数据的基准内和第二势垒高度,激发能的裂变异构体和半衰期在一组选定的钚,Cm,Cf,Fm,没有,Rf,Sg,Hs和F1核。结果也与Gogny-D1 M能量密度泛函得到的结果进行了比较。详细研究了原子序数为100 $\le$ Z $\le$ 126的同位素链的最小能量裂变路径,其中包括来自双中子滴线的高达约4 MeV的非常富中子的扇区。还讨论了单粒子能量、基态变形、配对相关、两核子分离能和势垒高度。除了裂变路径外,受约束的哈特里-福克-博戈留博夫框架还提供了集体质量和零点量子转动能和振动能。这些量是用于评估自发裂变半衰期t $_\mathrm{SF}$的系统性的Wentzel-Kramer-Brillouin形式主义内的构建块。通过对Viola-Seaborg公式进行参数化,计算$α$衰变半衰期t $_\mathrmα$,研究了自发裂变与$α$衰变之间的竞争.通过与已有实验数据和其它理论方法的比较,得出结论:D1 M $^{*}$是描述重核和超重核裂变的一个合理的出发点。

英文摘要:

The constrained Hartree-Fock-Bogoliubov approximation, based on the recent parametrization D1M$^{*}$ of the Gogny energy density functional, is used to describe fission in 435 superheavy nuclei. The Gogny-D1M$^{*}$ parametrization is benchmarked against available experimental data on inner and second barrier heights, excitation energies of the fission isomers and half-lives in a selected set of Pu, Cm, Cf, Fm, No, Rf, Sg, Hs and Fl nuclei. Results are also compared with those obtained with the Gogny-D1M energy density functional. A detailed study of the minimal energy fission paths is carried out for isotopic chains with atomic numbers 100 $\le$ Z $\le$ 126 including very neutron-rich sectors up to around 4 MeV from the two-neutron driplines. Single-particle energies, ground state deformations, pairing correlations, two-nucleon separation energies and barrier heights are also discussed. In addition to fission paths, the constrained Hartree-Fock-Bogoliubov framework provides collective masses and zero-point quantum rotational and vibrational energies. Those quantities are building blocks within the Wentzel-Kramer-Brillouin formalism employed to evaluate the systematic of the spontaneous fission half-lives t$_\mathrm{SF}$. The competition between spontaneous fission and $α$-decay is studied, through the computation of the $α$-decay half-lives t$_\mathrmα$ using a parametrization of the Viola-Seaborg formula. From the comparison with the available experimental data and the results obtained with other theoretical approaches, it is concluded that D1M$^{*}$ represents a reasonable starting point to describe fission in heavy and superheavy nuclei.

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