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Considering the Light Nuclei in the Cluster Model from NU Method

机译:从NU方法考虑聚类模型中的光核

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In this work, the energy levels of light nuclei from the NU method are calculated and their structures are determined. Therefore, by using a local potential that is suitable for light nuclei and compatible with the Hafstad-Teller potential, the Schrodinger equation from NU method is solved and the energy levels and wave functions are obtained. For more accuracy, the spin-orbit and tensor potentials are added to the central potential as perturbation and the first-order energy correction is obtained for the different states of many alpha systems. So, we calculate the energy levels of nuclei ~8Be and ~(16)O and compare the obtained results with the experimental data and get a good agreement. This agreement is better for ~(16)O than ~8Be. Therefore, anybody can conclude that the α cluster model has the better results for the nuclei with the number of more alpha particles. Finally, by the strength of Coulomb's repulsion, it is shown that the ground and first excited states of the ~(16)O nucleus have the tetrahedral and square configurations, respectively. Also, it is obtained that the structures of the second and third excited states are as square and linear chain that these structures show the non-localized gas configuration for the higher excited states of ~(16)O nucleus.
机译:在这项工作中,计算了来自NU方法的轻核的能级,并确定了它们的结构。因此,通过使用适合于光核并与Hafstad-Teller势兼容的局部势,可以解决NU方法的Schrodinger方程,并获得能级和波函数。为了获得更高的精度,将自旋轨道和张量势作为扰动添加到中心势,并且针对许多alpha系统的不同状态获得一阶能量校正。因此,我们计算了〜8Be和〜(16)O原子核的能级,并将获得的结果与实验数据进行比较,并获得了良好的一致性。该协议对于〜(16)O比〜8Be更好。因此,任何人都可以得出结论,对于具有更多α粒子数量的原子核,α团簇模型具有更好的结果。最后,通过库仑排斥的强度,表明〜(16)O核的基态和第一激发态分别具有四面体和方形构型。而且,获得的第二和第三激发态的结构是正方形和线性链,这些结构显示出〜(16)O核的更高激发态的非局部气体构型。

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