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The many relationships between the IBM and the Bohr model

机译:IBM和Bohr模型之间的许多关系

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Relationships between the IBM-1 and the Bohr collective model are explored in which the states of the IBM in its various dynamical symmetry limits are identified with subsets of Bohr model states of corresponding dynamical symmetries. The maps of interest are ones which give the contractions of the IBM in the limit of large boson number. The known map from the IBM into the Bohr model gives a contraction appropriate for the U(5) dynamical symmetry limit. A new map is given consistent with a contraction of the O(6) dynamical symmetry of the IBM. This map gives an explicit identification of IBM states in an O(6) superset of O(5) basis with states of the Wilets-Jean model and makes it possible to benefit from the different but complementary perspectives of the two models. For example, it leads to explicit expressions for the matrix elements of an IBM O(6) irrep in terms of the known matrix elements of the corresponding Wilets-Jean model. The relationship also shows how to obtain the familiar rotor plus beta- and gamma-vibrational bands of the Bohr-Mottelson model, in the IBM, by the addition to an O(6) Hamiltonian of a scalar cubic in the quadrupole moment operators of the type considered recently by Van Isacker. The establishment of close relationships between the two models enables one to benefit from the different and complementary perspectives they afford. For example, recent developments of an algebraic version of the collective model has shown that the Bohr model has an SU(1, 1) x O(5) dynamical group with representations ranging from those of a spherical vibrator to a beta-vibrational soft-gamma rotor of the Wilets-Jean limit and, with the addition of an interaction, to a rotor of the standard Bohr-Mottelson type with beta- and gamma-vibrational bands.
机译:探索了IBM-1和Bohr集体模型之间的关系,其中IBM处于其各种动态对称性极限中的状态通过相应动态对称性的Bohr模型状态子集进行标识。感兴趣的图是在大玻色子数的范围内给出IBM收缩的图。从IBM到Bohr模型的已知映射给出了适合U(5)动态对称极限的收缩。给出了与IBM的O(6)动态对称性收缩一致的新映射。该图以Wilets-Jean模型的状态在O(5)的O(6)的超集中给出了IBM状态的明确标识,并有可能从两个模型的不同但互补的角度受益。例如,根据对应的Wilets-Jean模型的已知矩阵元素,它导致IBM O(6)irrep矩阵元素的显式表达式。该关系还显示了如何通过在IBM的四极矩算符的标量三次方程的O(6)哈密顿量基础上,获得IBM熟悉的Bohr-Mottelson模型的转子以及β和γ振动带。 Van Isacker最近考虑的类型。两种模型之间建立紧密的关系使人们可以从它们提供的不同和互补的观点中受益。例如,集体模型的代数形式的最新发展表明,玻尔模型具有SU(1,1)x O(5)动力学组,其表示形式从球形振动器到β振动软- Wilets-Jean极限的γ转子,并加上相互作用后,成为具有β和γ振动带的标准Bohr-Mottelson型转子。

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