B<overline>0 → <overline>K(*)0X, B-- K(*) -X, B<overline>0s-η(η1;φ)X from the X(3872) molecular perspective

被引：1
|
作者：
Liang, Wei -Hong [1 ,2 ]
Ban, Ting [1 ]
Oset, Eulogio [1 ,3 ,4 ]
机构：
[1] Guangxi Normal Univ, Dept Phys, Guilin 541004, Peoples R China
[2] Guangxi Normal Univ, Guangxi Key Lab Nucl Phys & Technol, Guilin 541004, Peoples R China
[3] Univ Valencia, Ctr Mixto, Inst Invest Paterna, Dept Fis Teor,CSIC, Apartado 22085, Valencia 46071, Spain
[4] Univ Valencia, Ctr Mixto, IFIC, CSIC,Inst Invest Paterna, Apartado 22085, Valencia 46071, Spain
来源：
PHYSICAL REVIEW D | 2024年 / 109卷 / 05期
基金：
中国国家自然科学基金; 欧盟地平线“2020”;
关键词：
DECAYS; STATES;
D O I：
10.1103/PhysRevD.109.054030
中图分类号：
P1 [天文学];
学科分类号：
0704 ;
摘要：
We study the decays B over bar 0 - over bar K0X, B- - K-X, B over bar 0s - eta(eta 1)X, B over bar 0 - over bar K*0X, B- - K*-X, B over bar 0s - phi X, with X equivalent to X(3872), from the perspective of the X(3872) being a molecular state made from the interaction of the D*+D-; D*0 over bar D0, and c:c: components. We consider both the external and internal emission decay mechanisms and find an explanation for the over bar K0X and K-X production rates, based on the mass difference of the charged and neutral D*D over bar components. We also find that the internal and external emission mechanisms add constructively in the B over bar 0 - over bar K0X, B- - K-X reactions, while they add destructively in the case of widths of the present measurements and allows us to make predictions for the unmeasured modes of B over bar 0s - eta(eta 1)X(3872) and B- - K*-X(3872). The future measurement of these decay modes will help us get a better perspective on the nature of the X(3872) and the mechanisms present in production reactions of that state. B over bar 0 - over bar K*0X, B- - K*-X reactions. This feature explains the decay
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页数：9
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