强、弱电相互作用在理解核结合能表中的联合作用

Seshavatharam U V S, L. S
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引用次数: 2

摘要

人们试图把原子核模型化为束缚核子和自由核子或未束缚核子的组合。由于强相互作用,束缚核子有助于增加核结合能,而由于电弱相互作用,自由或未束缚核子有助于降低核结合能。在此背景下,我们参照4G最终统一和强相互作用模型,建立了一个统一的核结合能方案,该方案包含四个简单项,一个能量系数为10.1 MeV,两个小数字为0.0016和0.0019。在本文中,通过消除0.0019这个数字,我们试图微调属于能量系数为11.9 MeV的第二项的自由核子或未结合核子数的估计过程。有趣的观察是,Z可以被认为是Z的束缚同位素数目范围的特征表示。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
On the Combined Role of Strong and Electroweak Interactions in Understanding Nuclear Binding Energy Scheme
An attempt is made toa model the atomic nucleus as a combination of bound and free or unbound nucleons. Due to strong interaction, bound nucleons help in increasing nuclear binding energy and due to electroweak interaction, free or unbound nucleons help in decreasing nuclear binding energy. In this context, with reference to proposed 4G model of final unification and strong interaction, recently we have developed a unified nuclear binding energy scheme with four simple terms, one energy coefficient of 10.1 MeV and two small numbers 0.0016 and 0.0019. In this paper, by eliminating the number 0.0019, we try to fine tune the estimation procedure of number of free or unbound nucleons pertaining to the second term with an energy coefficient of 11.9 MeV. Interesting observation is that, Z can be considered as a characteristic representation of range of number of bound isotopes of  Z. 
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