Three-cluster equation using the two-cluster RGM kernel

被引:38
|
作者
Fujiwara, Y [1 ]
Nemura, H
Suzuki, Y
Miyagawa, K
Kohno, M
机构
[1] Kyoto Univ, Dept Phys, Kyoto 6068502, Japan
[2] KEK, Inst Nucl & Particle Phys, Tsukuba, Ibaraki 3050801, Japan
[3] Niigata Univ, Dept Phys, Niigata 9502181, Japan
[4] Okayama Univ Sci, Dept Appl Phys, Okayama 7000005, Japan
[5] Kyushu Dent Coll, Div Phys, Kitakyushu, Fukuoka 8038580, Japan
来源
PROGRESS OF THEORETICAL PHYSICS | 2002年 / 107卷 / 04期
关键词
D O I
10.1143/PTP.107.745
中图分类号
O4 [物理学];
学科分类号
0702 ;
摘要
We propose a new type of three-cluster equation which uses two-cluster resonating-group-method (RGM) kernels. In this equation, the orthogonality of the total wave function to two-cluster Pauli-forbidden states is essential to eliminate redundant components admixed in the three-cluster systems. The explicit energy dependence inherent in the exchange RGM kernel is self-consistently determined. For bound-state problems, this equation is straightforwardly transformed into the Faddeev equation, which uses a modified singularity-free T-matrix constructed from the two-cluster RGM kernel. The approximation of the present three-cluster formalism can be examined with a more complete calculation using the three-cluster RGM, As a simple example, we discuss three di-neutron (3d') and 3alpha systems in the harmonic-oscillator variational calculation. The result of the Faddeev calculation is also presented for the 3d' system.
引用
收藏
页码:745 / 757
页数:13
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