-
Abstract
The structure of H dihyperon (DH) is investigated by employing the SU (3) chiral quark model. As the structure of DH, two different configuations, six-quark cluster configuration and two-cluster configuration, are considered, respectively. The result shows that except the σ chiral field, the overall effect of the other SU (3) chiral fields is destructive in forming a stable DH and the two-cluster configuration is the preferred structure. The resultant mass of DH in a three-coupled-channel calculation in the SU (3) chiral quark model is ranged from 2225 to 2234 MeV.
Article Text
-
-
-
About This Article
Cite this article:
SHEN Peng-Nian, ZHANG Zong-Ye, YU You-Wen, YUAN Xiu-Qing, YANG Shu. Structure of H-Dihyperon[J]. Chin. Phys. Lett., 2000, 17(1): 7-9.
SHEN Peng-Nian, ZHANG Zong-Ye, YU You-Wen, YUAN Xiu-Qing, YANG Shu. Structure of H-Dihyperon[J]. Chin. Phys. Lett., 2000, 17(1): 7-9.
|
SHEN Peng-Nian, ZHANG Zong-Ye, YU You-Wen, YUAN Xiu-Qing, YANG Shu. Structure of H-Dihyperon[J]. Chin. Phys. Lett., 2000, 17(1): 7-9.
SHEN Peng-Nian, ZHANG Zong-Ye, YU You-Wen, YUAN Xiu-Qing, YANG Shu. Structure of H-Dihyperon[J]. Chin. Phys. Lett., 2000, 17(1): 7-9.
|