This title appears in the Scientific Report :
2015
Please use the identifier:
http://dx.doi.org/10.1016/j.physletb.2014.11.030 in citations.
Please use the identifier: http://hdl.handle.net/2128/9793 in citations.
Production of the spin partner of the $X\left(3872\right)$ in ${e}^{+}{e}^{-}$ collisions
Production of the spin partner of the $X\left(3872\right)$ in ${e}^{+}{e}^{-}$ collisions
We study the production of the spin partner of the X(3872), which is a D^{*}\bar D^{*} bound state with quantum numbers J^{PC}=2^{++} and named X_2(4012) here, with the associated emission of a photon in electron--positron collisions. The results show that the ideal energy region to observe the X_2(...
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Personal Name(s): | Guo, Feng-Kun (Corresponding author) |
---|---|
Meißner, Ulf-G. / Yang, Zhi | |
Contributing Institute: |
Theorie der Starken Wechselwirkung; IAS-4 Theorie der starken Wechselwirkung; IKP-3 |
Published in: | Physics letters / B, 740 (2015) S. 42 - 45 |
Imprint: |
Amsterdam
North-Holland Publ.
2015
|
DOI: |
10.1016/j.physletb.2014.11.030 |
Document Type: |
Journal Article |
Research Program: |
TRR 110: Symmetrien und Strukturbildung in der Quantenchromodynamik Computational Science and Mathematical Methods |
Link: |
OpenAccess OpenAccess |
Publikationsportal JuSER |
Please use the identifier: http://hdl.handle.net/2128/9793 in citations.
We study the production of the spin partner of the X(3872), which is a D^{*}\bar D^{*} bound state with quantum numbers J^{PC}=2^{++} and named X_2(4012) here, with the associated emission of a photon in electron--positron collisions. The results show that the ideal energy region to observe the X_2(4012) in e^+e^- annihilations is from 4.4~GeV to 4.5~GeV, due to the presence of the S-wave \bar D^{*} D_1(2420) and \bar D^{*} D_2(2460) thresholds, respectively. We also point out that it will be difficult to observe the \gamma X(4012) at the e^+e^- center-of-mass energy around 4.26~GeV. |