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Ablikim, M.; Bai, J. Z.; Ban, Y.; Bian, J. G.; X, Cai; Chang, J. F.; Chen, H. F.; Chen, H. S.; Chen, H. X.; Chen, J. C.; Chen, Jin; Chen, Jun; Chen, M. L.; Chen, Y. B.; Chi, S. P.; Chu, Y. P.; Cui, X. Z.; Dai, H. L.; Dai, Y. S.; Deng, Z. Y.; Liu, Dong; Dong, Qingshun; Du, S. X.; Du, Z. Z.; Fang, J.; Fang, S. S.; Fu, C. D.; Fu, Hai-Bing; Gao, C. S.; Gao, Yang; Gong, Ming; Gong, W. X.; Gu, S.; Guo, Y. N.; Guo, Y. Q.; Guo, Z. J.; Harris, F. A.; He, K. L.; He, Miao; He, Xiao‐Gang; Heng, Y. K.; Hu, H. M.; Hu, T.; Huang, G. S.; Huang, X. P.; Huang, X. T.; Ji, Xiangdong; Jiang, C. H.; Jiang, X. S.; Jin, D. P.; Jin, S.; Jin, Y.; Lai, Y. F.; Li, Feng; Li, Guanxin; Li, H. H.; Li, Jiaxun; Li, J. C.; Li, Q. J.; Li, R. Y.; Li, S. M.; Li, W. D.; Li, W. G.; Li, X. L.; Li, X. Q.; Li, Yaxue; Liang, Y. F.; Liao, H.; Liu, Chao; Liu, F.; Liu, Fang; Liu, H. H.; LIU, Hongzheng; Liu, J.; Liu, J. B.; Liu, J. P.; Liu, R. G.; Liu, Z. A.; Liu, Zhihong; Lu, F. X.; Lu, G. R.; Lü, H. J.; Lu, J. G.; Luo, C. L.; Luo, Liying; Luo, X. L.; C., F.; L., H.; M., J.; L., L.; M., Q.; B., X.; Y., X.; Mao, Z. P.; Mo, X. H.; Nie, J.; Nie, Z. D.; Olsen, S. L.; Peng, H.; Qi, N. D.; Qian, C. D.; H, Qin; Qiu, J. F.; Ren, Z.; Rong, G.; Shan, L. Y.; Shang, L.; Shen, D. L.; Shen, X. Y.; Sheng, H. Y.; Shi, Feng; Shi, X.; Sun, H.; Sun, J. F.; Sun, S. S.; Sun, Y. Z.; Sun, Z. J.; Tang, X.; Tao, N.; Tian, Yang; Tong, G. L.; Varner, G.; Wang, D. Y.; Wang, J. Z.; Wang, K.; WANG, Longye; Wang, L. S.; Wang, Meng; Wang, P.; Wang, P. L.; Wang, Sizhe; Wang, W. F.; Wang, Y. F.; Wang, Z.; Wang, Z. Y.; Wang, Zhe; Wang, Zheng; Wei, C.; Wei, D. H.; Wu, N.; Wu, Y. M.; Xia, X. M.; Xie, X. X.; Xin, B.; Xu, G. F.; Xu, H. Y.; Xue, S.; Yan, Mu-Lin; Yang, F.; Yang, H. X.; Yang, J.; Yang, Yifan; Ye, M.; Ye, M. H.; Ye, Y. X.; Yi, L. H.; Yi, Z. Y.; Chen, Yu; Yu, G.; Yuan, C. Z.; Yuan, J. M.; Yuan, Y.; Zang, S. L.; Zeng, Y.; Zhang, B. X.; Zhang, B. Y.; Zhang, C. C.; Zhang, D. H.; Zhang, H. Y.; Zhang, J.; Zhang, J. W.; Zhang, J. Y.; Zhang, Q. J.; Zhang, S. Q.; Zhang, Xing; Zhang, Xiran; Zhang, Yuxuan; Zhang, Yiyun; Zhang, Zhenzuo; Zhang, Z. Q.; Zhao, Dongxu; Zhao, J. B.; Zhao, Jiawei; Zhao, M. G.; Zhao, P. P.; Zhao, W. R.; Zhao, Xinli; Zhao, Y. B.; Zhao, Z.; Zheng, H. Q.; Zheng, J. P.; Zheng, Lei; Zheng, Z. P.; Zhong, X. C.; Zhou, B.; Zhou, G. M.; Li, Zhou; Zhou, Na; Zhu, K. J.; Zhu, Q. M.; Zhu, Y. S.; Zhu, Y.; Zhu, Z. A.; Zhuang, B. A.; Zhuang, X.; Zou, B. S.

doi:10.1103/physrevd.71.032003

Cited by 14 publications

(1 citation statement)

References 19 publications

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“…There, it is shown that although the EM contributions to J /ψ → V P are generally small relative to the strong decays as found by many other studies [20], they may turn out to be more competitive in ψ → V P compared with ψ → 3g → V P amplitudes, and produce crucial interferences [19]. For a better understanding of the 'ρπ puzzle', a thorough study of J /ψ(ψ ) → V P including both strong and EM transitions and accommodating up-to-date experimental information [21][22][23][24] should be necessary.…”

Section: Introductionmentioning

confidence: 92%

Decays ofJ/ψ and ψ′ into vector and pseudoscalar mesons and the pseudoscalar glueball–q\bar{q} mixing

Li¹,

Zhao²,

Chang³

2008

J. Phys. G: Nucl. Part. Phys.

104

165

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We introduce a parametrization scheme for J/ψ(ψ ′ ) → V P where the effects of SU(3) flavor symmetry breaking and doubly OZI-rule violation (DOZI) can be parametrized by certain parameters with explicit physical interpretations. This scheme can be used to clarify the glueball-q q mixing within the pseudoscalar mesons. We also include the contributions from the electromagnetic (EM) decays of J/ψ and ψ ′ via J/ψ(ψ ′ ) → γ * → V P . Via study of the isospin violated channels, such as J/ψ(ψ ′ ) → ρη, ρη ′ , ωπ 0 and φπ 0 , reasonable constraints on the EM decay contributions are obtained. With the up-to-date experimental data for J/ψ(ψ ′ ) → V P , J/ψ(ψ ′ ) → γP and P → γγ, etc, we arrive at a consistent description of the mentioned processes with a minimal set of parameters. As a consequence, we find that there exists an overall suppression of the ψ ′ → 3g form factors, which sheds some light on the long-standing "ρπ puzzle". By determining the glueball components inside the pseudoscalar η and η ′ in three different glueball-q q mixing schemes, we deduce that the lowest pseudoscalar glueball, if exists, has rather small q q component, and it makes the η(1405) a preferable candidate for 0 −+ glueball.

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