中国科学技术大学学报 ›› 2016, Vol. 46 ›› Issue (7): 574-579.DOI: 10.3969/j.issn.0253-2778.2016.07.006

• 原创论文 • 上一篇    下一篇

走近 X(3872) 共振态的本质

ACHASOV N. N.   

  1. 1.索博列夫数学学院理论物理实验室,新西伯利亚 630090,俄罗斯; 2.新西伯利亚州立大学,新西伯利亚 630090,俄罗斯
  • 收稿日期:2015-11-30 修回日期:2016-04-20 出版日期:2016-07-31 发布日期:2016-07-31
  • 作者简介:ACHASOV N. N. (corresponding author), male, born in 1941, Prof. Research field: high energy physics.

Towards the nature of X(3872) resonance

ACHASOV N. N.   

  1. 1.Laboratory of Theoretical Physics, Sobolev Institute for Mathematics, Novosibirsk 630090, Russian; 2.Novosibirsk State University, Novosibirsk 630090, Russian
  • Received:2015-11-30 Revised:2016-04-20 Online:2016-07-31 Published:2016-07-31
  • Contact: ACHASOV N. N.

摘要: 构造了具有良好解析性和幺正性的共振态X(3872)衰变谱,能够定义衰变反应X(3872)→D*0D0+c.c.的分支比,而只需要多研究另外一个衰变,比如说X(3872)→π+π-J/ψ(1S)衰变,这表明构造谱是筛选共振态X(3872)模型的有效工具.之后讨论了共振态X(3872)是粲偶素c=χc1(2P)的情形,此时它处在D*0D0的阈上.根据由粲偶素χc1(2P)的质量的势能模型的预言解释了共振态X(3872)的质量偏移.这个势能模型是依据衰变产物D*D+c.c.的中间态计入共振态X(3872)的质量的贡献而构造的.这使得我们能够研究共振态X(3872)和衰变道D*0D0的耦合常数,X(3872)→D*0D0+c.c.的衰变分支比以及共振态X(3872)衰变到所有不含D*0D0+c.c.的过程的分支比.预言了一个共振态X(3872)通过双胶子衰变的重要常数.

关键词: 粲偶素, 分子, 双胶子衰变

Abstract: The spectra of decays of resonance X(3872) with good analytical and unitary properties are constructed, which allows to define the branching ratio of the X(3872)→D*0D0+c.c. decay by studying only one more decay, for example, the X(3872)→π+π-J/ψ(1S) decay, and it is shown that the spectra are an effective means of selection of models for the resonance X(3872). Then the scenario is discussed where the X(3872) resonance is the c=χc1(2P) charmonium which “sits on” the D*0D0 threshold. An explanation is given of the shift of the mass of the X(3872) resonance with respect to the prediction of a potential model for the mass of the χc1(2P) charmonium by the contribution of the virtual D*D+c.c. intermediate states into the self energy of the X(3872) resonance. This allows us to estimate the coupling constant of the X(3872) resonance with the D*0D0 channel, the branching ratio of the X(3872)→D*0D0+c.c. decay, and the branching ratio of the X(3872) decay into all non-D*0D0+c.c. states. A significant number of unknown decays of X(3872) via two gluons: X(3872)→gluon gluon→hadrons are predicted.

Key words: Charmonium, molecule, two-gluon decays