Nature of X(6900) and its production mechanism at LHCb
We show that the Pomeron exchanges play a unique role in vector charmonium scatterings. Such a mechanism can provide a natural explanation for the nontrivial structures in the di-J/ψ spectrum observed by the LHCb Collaboration. The narrow structure X(6900), as a dynamically generated resonance pole,...
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2022
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oai:doaj.org-article:7cc369f71e404a28af2b5a71ecbbc44a2021-12-04T04:32:47ZNature of X(6900) and its production mechanism at LHCb0370-269310.1016/j.physletb.2021.136794https://doaj.org/article/7cc369f71e404a28af2b5a71ecbbc44a2022-01-01T00:00:00Zhttp://www.sciencedirect.com/science/article/pii/S0370269321007346https://doaj.org/toc/0370-2693We show that the Pomeron exchanges play a unique role in vector charmonium scatterings. Such a mechanism can provide a natural explanation for the nontrivial structures in the di-J/ψ spectrum observed by the LHCb Collaboration. The narrow structure X(6900), as a dynamically generated resonance pole, can arise from the Pomeron exchanges and coupled-channel effects between the J/ψ-J/ψ, J/ψ-ψ(2S) scatterings. A pole structure near the di-J/ψ threshold is also found. Meanwhile, we predict that X(6900) can produce significant threshold enhancement in the J/ψ-ψ(2S) energy spectrum which can be searched for at LHCb.Chang GongMeng-Chuan DuQiang ZhaoXian-Hui ZhongBin ZhouElsevierarticlePhysicsQC1-999ENPhysics Letters B, Vol 824, Iss , Pp 136794- (2022) |
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Physics QC1-999 |
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Physics QC1-999 Chang Gong Meng-Chuan Du Qiang Zhao Xian-Hui Zhong Bin Zhou Nature of X(6900) and its production mechanism at LHCb |
description |
We show that the Pomeron exchanges play a unique role in vector charmonium scatterings. Such a mechanism can provide a natural explanation for the nontrivial structures in the di-J/ψ spectrum observed by the LHCb Collaboration. The narrow structure X(6900), as a dynamically generated resonance pole, can arise from the Pomeron exchanges and coupled-channel effects between the J/ψ-J/ψ, J/ψ-ψ(2S) scatterings. A pole structure near the di-J/ψ threshold is also found. Meanwhile, we predict that X(6900) can produce significant threshold enhancement in the J/ψ-ψ(2S) energy spectrum which can be searched for at LHCb. |
format |
article |
author |
Chang Gong Meng-Chuan Du Qiang Zhao Xian-Hui Zhong Bin Zhou |
author_facet |
Chang Gong Meng-Chuan Du Qiang Zhao Xian-Hui Zhong Bin Zhou |
author_sort |
Chang Gong |
title |
Nature of X(6900) and its production mechanism at LHCb |
title_short |
Nature of X(6900) and its production mechanism at LHCb |
title_full |
Nature of X(6900) and its production mechanism at LHCb |
title_fullStr |
Nature of X(6900) and its production mechanism at LHCb |
title_full_unstemmed |
Nature of X(6900) and its production mechanism at LHCb |
title_sort |
nature of x(6900) and its production mechanism at lhcb |
publisher |
Elsevier |
publishDate |
2022 |
url |
https://doaj.org/article/7cc369f71e404a28af2b5a71ecbbc44a |
work_keys_str_mv |
AT changgong natureofx6900anditsproductionmechanismatlhcb AT mengchuandu natureofx6900anditsproductionmechanismatlhcb AT qiangzhao natureofx6900anditsproductionmechanismatlhcb AT xianhuizhong natureofx6900anditsproductionmechanismatlhcb AT binzhou natureofx6900anditsproductionmechanismatlhcb |
_version_ |
1718373039845933056 |