Direct pion emission in D*+→D+π decays

  • The QCD multipole expansion (QCDME) is based on quantum field theory and has been extensively applied to study transitions among Υ and ψ family members. As it refers to non-perturbative QCD, however, it has only a certain application range. Even though it successfully explains the transition data among members of the Υ (ψ) family, as Eichten indicates, beyond the production threshold of mediate states it fails to match data by several orders of magnitude. In this work, by studying a simple decay mode D*→D+π0, where a pion may be emitted before D* transitions into D, we analyze the contribution of QCD multipole expansion. As the Dπ portal is open, the dominant contribution is an OZI-allowed process where a light quark-pair is excited out from vacuum, and its contribution can be evaluated by the 3P0 model. Since direct pion emission is OZI-suppressed and violates isospin conservation, its contribution must be much smaller than the dominant one. By a careful calculation, we estimate that the QCDME contribution should be 3-4 orders smaller than the dominant contribution and this result can offer a quantitative interpretation for Eichten's statement.
      PCAS:
  • 加载中
  • [1] Y. P. Kuang and T. M. Yan, Phys. Rev. D, 24:2874(1981)
    [2] T. M. Yan, Phys. Rev. D, 22:1652(1980)
    [3] L. Micu, Nucl. Phys. B, 10:521(1969)
    [4] A. Le Yaouanc, L. Oliver, O. Pne and J. Raynal, Phys. Rev. D, 8:2223(1973); 9:1415(1974); 11:1272(1975); Phys. lett. B, 71:57(1977); 71:397(1977)
    [5] A. Le Yaouanc, L. Oliver, O. Pne and J. Raynal, Phys. Lett. B, 72:57(1977)
    [6] A. Le Yaouanc, L. Oliver, O. Pne and J. Raynal, Hadron Transitions in the Quark Model, Gordon and Breach Science Publishers, New York, 1987
    [7] E. van Beveren, C. Dullemond and G. Rupp, Phys. Rev. D, 21:772(1980); E. van Beveren, G. Rupp, T.A. Rijken and C. Dullemond, Phys. Rev. D, 27:1527(1983)
    [8] R. Bonnaz, B. Silvestre-Brac and C. Gignoux, Eur. Phys. J. A, 13:363-376(2002)
    [9] W. Roberts and B. Silvestre-Brac, Few-Body Systems, 11, 171(1992)
    [10] H.G. Blundell and S. Godfrey, Phys. Rev. D, 53:3700(1996)
    [11] P.R. Page, Nucl. Phys. B, 446:189(1995); S. Capstick and N. Isgur, Phys. Rev. D, 34:2809(1986)
    [12] S. Capstick and W. Roberts, Phys. Rev. D, 49:4570(1994)
    [13] E.S. Ackleh, T. Barnes and E.S. Swanson, Phys. Rev. D, 54:6811(1996)
    [14] H.Q. Zhou, R.G. Ping and B.S. Zou, Phys. Lett. B, 611:123(2005)
    [15] X.H. Guo, H.W. Ke, X.Q. Li, X. Liu and S.M. Zhao, Commun. Theor. Phys., 48:509-518(2007)
    [16] F. E. Close and E. S. Swanson, Phys. Rev. D, 72:094004(2005)[hep-ph/0505206]
    [17] J. Lu, W.Z. Deng, X.L. Chen and S.L. Zhu, Phys. Rev. D, 73:054012, (2006)
    [18] B. Zhang, X. Liu, W.Z. Deng and S.L. Zhu, Eur. Phys. J. C, 50:617(2007)
    [19] C. Chen, X.L. Chen, X. Liu, W.Z. Deng and S.L. Zhu, Phys. Rev. D, 75:094017(2007); X. Liu, C. Chen, W.Z. Deng and X.L. Chen, Chin. Phys. C, 32:424-427(2008), arXiv:0710.0187[hep-ph].
    [20] D. M. Li and B. Ma, Phys. Rev. D, 77:074004(2008); D. M. Li and B. Ma, Phys. Rev. D, 77:094021(2008); D. M. Li and S. Zhou, Phys. Rev. D, 78:054013(2008); D. M. Li and S. Zhou, arXiv:0811.0918[hep-ph]
    [21] Z. Y. Zhou and Z. Xiao, Phys. Rev. D, 84:034023(2011) doi:10.1103/PhysRevD.84.034023[arXiv:1105.6025[hep-ph]]
    [22] H. G. Blundell and S. Godfrey, Phys. Rev. D, 53:3700(1996)[hep-ph/9508264]
    [23] K. A. Olive et al (Particle Data Group Collaboration), Chin. Phys. C 38, 090001(2014)
    [24] R. Casalbuoni, A. Deandrea, N. Di Bartolomeo, R. Gatto, F. Feruglio and G. Nardulli, Phys. Rept. 281, 145(1997)[hep-ph/9605342]
    [25] Y. P. Kuang, Front. Phys. China 1, 19(2006)[hep-ph/0601044]
    [26] Y. P. Kuang, S. F. Tuan and T. M. Yan, Phys. Rev. D, 37:1210(1988)
    [27] Y. P. Kuang, Y. P. Yi and B. Fu, Phys. Rev. D, 42:2300(1990)
    [28] J. B. Liu and M. Z. Yang, JHEP, 1407:106(2014)[arXiv:1307.4636[hep-ph]]
    [29] H. W. Ke, J. Tang, X. Q. Hao and X. Q. Li, Phys. Rev. D, 76:074035(2007)[arXiv:0706.2074[hep-ph]]; H. W. Ke and X. Q. Li, Sci. China Phys. Mech. Astron., 53:2019(2010)[arXiv:0910.1158[hep-ph]]
    [30] C. Meng and K. T. Chao, Phys. Rev. D, 78:074001(2008)[arXiv:0806.3259[hep-ph]]
    [31] F. K. Guo, P. N. Shen, H. C. Chiang and R. G. Ping, Phys. Lett. B, 658:27(2007)[hep-ph/0601120]
  • 加载中

Get Citation
Xing-Dao Guo, Xue-Wen Liu, Hong-Wei Ke and Xue-Qian Li. Direct pion emission in D*+→D+π decays[J]. Chinese Physics C, 2016, 40(7): 073103. doi: 10.1088/1674-1137/40/7/073103
Xing-Dao Guo, Xue-Wen Liu, Hong-Wei Ke and Xue-Qian Li. Direct pion emission in D*+→D+π decays[J]. Chinese Physics C, 2016, 40(7): 073103.  doi: 10.1088/1674-1137/40/7/073103 shu
Milestone
Received: 2015-11-17
Fund

    Supported by National Natural Science Foundation of China (11375128)

Article Metric

Article Views(1756)
PDF Downloads(23)
Cited by(0)
Policy on re-use
To reuse of Open Access content published by CPC, for content published under the terms of the Creative Commons Attribution 3.0 license (“CC CY”), the users don’t need to request permission to copy, distribute and display the final published version of the article and to create derivative works, subject to appropriate attribution.
通讯作者: 陈斌, bchen63@163.com
  • 1. 

    沈阳化工大学材料科学与工程学院 沈阳 110142

  1. 本站搜索
  2. 百度学术搜索
  3. 万方数据库搜索
  4. CNKI搜索

Email This Article

Title:
Email:

Direct pion emission in D*+→D+π decays

    Corresponding author: Xing-Dao Guo,
    Corresponding author: Xue-Wen Liu,
    Corresponding author: Hong-Wei Ke,
    Corresponding author: Xue-Qian Li,
Fund Project:  Supported by National Natural Science Foundation of China (11375128)

Abstract: The QCD multipole expansion (QCDME) is based on quantum field theory and has been extensively applied to study transitions among Υ and ψ family members. As it refers to non-perturbative QCD, however, it has only a certain application range. Even though it successfully explains the transition data among members of the Υ (ψ) family, as Eichten indicates, beyond the production threshold of mediate states it fails to match data by several orders of magnitude. In this work, by studying a simple decay mode D*→D+π0, where a pion may be emitted before D* transitions into D, we analyze the contribution of QCD multipole expansion. As the Dπ portal is open, the dominant contribution is an OZI-allowed process where a light quark-pair is excited out from vacuum, and its contribution can be evaluated by the 3P0 model. Since direct pion emission is OZI-suppressed and violates isospin conservation, its contribution must be much smaller than the dominant one. By a careful calculation, we estimate that the QCDME contribution should be 3-4 orders smaller than the dominant contribution and this result can offer a quantitative interpretation for Eichten's statement.

    HTML

Reference (31)

目录

/

DownLoad:  Full-Size Img  PowerPoint
Return
Return