将s和d玻色子引入壳模型SU(3)波函数

A. Martinou
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引用次数: 0

摘要

壳模型SU(3)对称性是由Elliott在1958年发现的,从那时起它就成为了核壳模型的代数实现。它被认为是一个费米子核模型,因为它处理的是原子核占据轨道的问题。Elliott证明了核子在LS(自旋-轨道)耦合方案中存在SU(3)对称性。另一方面,Arima和Iachello在1975年提出了相互作用玻色子模型,它是一个玻色子模型。相互作用玻色子模型中的玻色子是由核子对推导出来的。但是核子对到玻色子的映射(Otsuka-Arima-Iachello映射)仅在jj耦合方案下是泛函数的,因此它只适用于相互作用玻色子模型的U(5)和O(6)极限。但是在相互作用玻色子模型的SU(3)极限中,s和d玻色子的起源是什么呢?在此,我证明了s和d玻色子存在于空间壳模型SU(3)波函数中,并且它们来自于谐振子量子对。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
The s and d bosons into the Shell Model SU(3) wave functions
The Shell Model SU(3) symmetry was discovered by Elliott in 1958 and since then has been the algebraic realization of the Nuclear Shell Model. It is considered to be a fermionic nuclear model, since it tackles with the occupancies of the orbitals by nucleons. Elliott proved that the SU(3) symmetry appears in the LS (spin-orbit) coupling scheme of the nucleons. On the other side the Interacting Boson Model was proposed by Arima and Iachello in 1975 and it is a boson model. The bosons in the Interacting Boson Model are being derived by nucleon pairs. But the mapping (Otsuka-Arima-Iachello mapping) of the nucleon pairs into bosons is functional only in the jj coupling scheme and so it is applicable only in the U(5) and O(6) limits of the Interacting Boson Model. But what is the origin of the s and d bosons in the SU(3) limit of the Interacting Boson Model? Hereby I demonstrate that the s and d bosons are present into the spatial Shell Model SU(3) wave functions and that they derive from pairs of harmonic oscillator quanta.
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