Coupled-channel analysis of the possible D(*)D(*), (B)over-bar(*)(B)over-bar(*) and D(*)(B)over-bar(*) molecular states

被引:105
|
作者
Li, Ning [1 ,2 ,3 ,4 ]
Sun, Zhi-Feng [5 ,6 ,7 ]
Liu, Xiang [5 ,6 ,7 ]
Zhu, Shi-Lin [1 ,2 ,8 ,9 ]
机构
[1] Peking Univ, Dept Phys, Beijing 100871, Peoples R China
[2] Peking Univ, State Key Lab Nucl Phys & Technol, Beijing 100871, Peoples R China
[3] Forschungszentrum Julich, Inst Kernphys, D-52425 Julich, Germany
[4] Forschungszentrum Julich, Julich Ctr Hadron Phys, D-52425 Julich, Germany
[5] Lanzhou Univ, Sch Phys Sci & Technol, Lanzhou 730000, Peoples R China
[6] Lanzhou Univ, Res Ctr Hadron & CSR Phys, Lanzhou 730000, Peoples R China
[7] Chinese Acad Sci, Inst Modern Phys, Lanzhou 730000, Peoples R China
[8] Peking Univ, Ctr High Energy Phys, Beijing 100871, Peoples R China
[9] Collaborat Innovat Ctr Quantum Matter, Beijing 100871, Peoples R China
来源
PHYSICAL REVIEW D | 2013年 / 88卷 / 11期
基金
中国国家自然科学基金;
关键词
CHIRAL PERTURBATION-THEORY; EXCITED HEAVY MESONS; CHARMONIUM; X(3872); DEUSONS;
D O I
10.1103/PhysRevD.88.114008
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
We perform a coupled-channel study of the possible deuteron-like molecules with two heavy flavor quarks, including the systems of D-(*D-)(()*()) with double charm, (B) over bar (()*())(B) over bar (()*()) with double bottom, and D-(*())(B) over bar (()*()) with both charm and bottom, within the one-boson-exchange potential model. In our study, we take into account the S-D mixing which plays an important role in the formation of the loosely bound deuteron, and particularly, the coupled-channel effect in the flavor space. According to our results, the state D-(*D-)(()*())[I(J(P)) = 0(1(+))] with double charm, the states (B) over bar (()*())(B) over bar (()*())[I(J(P)) = 0(1(+)), 1((+))], ((B) over bar (()*())(B) over bar (()*()))(s)[J(P) = 1(+), 2(+)] and ((B) over bar (()*())(B) over bar (()*()))(ss)[J(P) = 1(+), 2(+)] with double bottom, and the states D-(*())(B) over bar (()*())[I(J(P)) = 0(1(+)), 0(2(+))] with both charm and bottom might be good molecule candidates. However, the states D-(*D-)(()*())[I(J(P)) = 0(2(+)), 1(0(+)), 1(1(+)), 1(2(+))], (D-(*D-)(()*()))(s)[J(P) = 0(+), 2(+)] and (D-(*D-)(()*()))(ss)[J(P) = 0(+), 1(+), 2(+)] with double charm and the state D-(*())(B) over bar (()*())[I(J(P)) = 1(1(+))] with both charm and bottom are not supported to be molecules.
引用
收藏
页数:20
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