K* mesons with hidden charm arising from KX(3872) and KZc(3900) dynamics

被引:29
|
作者
Ren, Xiu-Lei [1 ]
Malabarb, Brenda B. [2 ]
Geng, Li-Sheng [3 ,4 ,5 ]
Khemchandani, K. P. [3 ,4 ,6 ]
Martinez Torres, A. [2 ,3 ,4 ]
机构
[1] Ruhr Univ Bochum, Inst Theoret Phys 2, D-44780 Bochum, Germany
[2] Univ Sao Paulo, Inst Fis, CP 66318, BR-05389970 Sao Paulo, SP, Brazil
[3] Beihang Univ, Sch Phys & Nucl Energy Engn, Beijing 100191, Peoples R China
[4] Beihang Univ, Beijing Key Lab Adv Nucl Mat & Phys, Beijing 100191, Peoples R China
[5] Beihang Univ, Beijing Adv Innovat Ctr Big Date Based Precis Med, Beijing 100191, Peoples R China
[6] Univ Fed Sao Paulo, CP 01302-907, Sao Paulo, Brazil
基金
中国国家自然科学基金; 巴西圣保罗研究基金会;
关键词
Exotic hadrons; Few body systems; Heavy quark symmetry; PENTAQUARK; DEUTERIUM; EXOTICS;
D O I
10.1016/j.physletb.2018.08.034
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
Inspired by the recent discovery of the pentaquark states P-c(4450) and P-c(4380), which can be viewed as excited nucleon states with hidden charm, we study the three-body interaction of a kaon and a pair of D (D) over bar* in isospin 0 and 1. We show that the two body interactions stringently constrained by the existence of the D-s0*(2317), D-s1*(2460), X(3872), and Z(c)(3900), which are widely believed to contain large DK, D*K, and D (D) over bar* components, inevitably lead to the existence of a heavy K* meson with hidden charm. Concrete coupled channel three-body calculations yield its mass and width as (4307 +/- 2) - i(9 +/- 2) MeV with I(J(P)) = 1/2(1(-)). This state, if found experimentally, definitely cannot be accommodated in a q (q) over bar picture, and therefore presents a clear case of an exotic hadron. (c) 2018 The Author(s). Published by Elsevier B.V. This is an open access article under the CC BY license.
引用
收藏
页码:112 / 117
页数:6
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