Wilsonian renormalization group analysis of nonrelativistic three-body systems without introducing dimerons

被引:2
|
作者
Harada, Koji [1 ]
Kubo, Hirofumi [2 ]
Yoshimoto, Issei [1 ]
机构
[1] Kyushu Univ, Dept Phys, Fukuoka 8128581, Japan
[2] Saga Univ, Synchrotron Light Applicat Ctr, Honjo, Saga 8408502, Japan
来源
PHYSICAL REVIEW D | 2013年 / 87卷 / 08期
关键词
EFFECTIVE-FIELD THEORY; 3-BOSON SYSTEM; EQUATION; FORCES; RG;
D O I
10.1103/PhysRevD.87.085006
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
Low-energy effective field theory describing a nonrelativistic three-body system is analyzed in the Wilsonian renormalization group method. No effective auxiliary field (dimeron) that corresponds to two-body propagation is introduced. The Efimov effect is expected in the case of an infinite two-body scattering length and is believed to be related to the limit cycle behavior in the three-body renormalization group equations (RGEs). If the one-loop property of the RGEs for the nonrelativistic system without the dimeron field, which is essential in deriving RGEs in the two-body sector, persists in the three-body sector, it appears to prevent the emergence of limit cycle behavior. We explain how the multiloop diagrams contribute in the three-body sector without contradicting the one-loop property of the RGEs and derive the correct RGEs, which lead to the limit cycle behavior. The Efimov parameter, s(0), is obtained within a few percent error in the leading orders. We also remark on the correct use of the dimeron formulation. We find rich renormalization group flow structure in the three-body sector. In particular, a novel nontrivial fixed point of the three-body couplings is found when the two-body interactions are absent. We also find, on the two-body nontrivial fixed point, the limit cycle is realized as a loop of finite size in the space of three-body coupling constants when terms with derivatives are included. DOI:10.1103/PhysRevD.87.085006
引用
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页数:19
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