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Chinese Physics C

BOSON REPRESENTATION OF THE k-LEVEL LIPKIN MODEL

Yt Yang, Xu Guo

Published Jan 1, 1987• 0 citations
OpenAlex

Abstract

The boson representation of k-level Lipkin model for a fermion system was given by usingthe theory of coherent states.The method discussed in this paper can be used not only for thek-level Lipkin model corresponding to S_P (2k) group,but also for other solvable model cor-responding to other semisimple Lie groups.It was pointed out that the norm operator is afunction of the Casimir operators of dynamical group and its maximum stationary subgroup.

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The boson representation of k-level Lipkin model for a fermion system was given by usingthe theory of coherent states.The method discussed in this paper can be used not only for thek-level Lipkin model corresponding to S_P (2k) group,but also for other solvable model cor-responding to other semisimple Lie groups.It was pointed out that the norm operator is afunction of the Casimir operators of dynamical group and its maximum stationary subgroup.
Following an idea, recently, proposed by the present authors for the two-level pairing model, the Lipkin model is reexamined. It is a natural generalization of the method already developed by the present authors with Kuriyama. This model is a schematic model for many-fermion systems and obeys the su(2)-algebra. It is shown that the use of the Schwinger boson representation, the model is expressed in terms of the su(1,1) ⊗ su(1,1)-algebra and with the aid of the MYT mapping method, it is disguised from the orginal form in terms of the Holstein-Primakoff representation. Further, under various coherent states, the classical counterparts are derived. It is concluded that the Lipkin model can be treated in the common ring as that of the two-level pairing model.
A new method for describing the two-level pairing model in a many-fermion system is presented. The basic idea comes from the Schwinger boson representation for the su(2) ⊗ su(2)-algebra, in which four kinds of boson operators govern the dynamics. It is well known that in the original fermion space, it is almost impossible to introduce any trial state for the variation except the BCS state in the framework of the mean field approximation. However, in the Schwinger boson representation, various trial states can be defined on the condition that the mean field approximation is useful. In these states, the su(2) ⊗ su(1,1)-coherent state is mainly discussed in this paper.
A new method for describing the two-level pairing model in a many-fermion system is presented. Basic idea comes from the Schwinger boson representation for the su(2) cross su(2)-algebra, in which four kinds of boson operators govern the dynamics. It is well known that in the original fermion space, it is almost impossible to introduce any trial state for the variation except the BCS state in the framework of the mean field approximation. However, in the Schwinger boson representation, various trial states can be defined on the condition that the mean field approximation is useful. In these states, the mixed-mode coherent state is mainly discussed in this paper.