Study ofX(5568) in a unitary coupled-channel approximationof BK and Bsπ

  • The potential of the m B meson and the pseudoscalar meson is constructed up to the next-to-leading order Lagrangian, and then the m B Kand m B sπ interaction is studied in the unitary coupled-channel approximation. A resonant state with a mass about 5568 MeV and J P=0 +is generated dynamically, which can be associated with the X(5568) state announced by the D0 Collaboration recently. The mass and the decay width of this resonant state depend on the regularization scale in the dimensional regularization scheme, or the maximum momentum in the momentum cutoff regularization scheme. The scattering amplitude of the vector Bmeson and the pseudoscalar meson is calculated, and an axial-vector state with a mass near 5620 MeV and J P=1 +is produced. Their partners in the charm sector are also discussed.
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  • [1] S. S. Agaev, K. Azizi and H. Sundu, Phys. Rev. D, 93: 074024 (2016)
    [2] V. M. Abazov et al (D0 Collaboration), Phys. Rev. Lett., 117:022003 (2016)
    [3] W. Wang and R. Zhu, Chin. Phys. C, 40: 093101 (2016)
    [4] Z. G. Wang, Commun. Theor. Phys., 66: 335 (2016)
    [5] W. Chen, H. X. Chen, X. Liu, T. G. Steele and S. L. Zhu, Phys. Rev. Lett., 117: 022002 (2016)
    [6] S. S. Agaev, K. Azizi and H. Sundu, Phys. Rev. D, 93: 114007 (2016)
    [7] X. H. Liu and G. Li, Eur. Phys. J. C, 76: 455 (2016)
    [8] Y. R. Liu, X. Liu and S. L. Zhu, Phys. Rev. D, 93: 074023 (2016)
    [9] S. S. Agaev, K. Azizi and H. Sundu, Phys. Rev. D, 93: 094006 (2016)
    [10] J. M. Dias, K. P. Khemchandani, A. Martnez Torres, M. Nielsen and C. M. Zanetti, Phys. Lett. B, 758: 235 (2016)
    [11] Z. G. Wang, Eur. Phys. J. C, 76: 279 (2016)
    [12] S. S. Agaev, K. Azizi and H. Sundu, Eur. Phys. J. Plus, 131:351 (2016)
    [13] X. G. He and P. Ko, Phys. Lett. B, 761: 92 (2016)
    [14] F. Stancu, J. Phys. G, 43: 105001 (2016)
    [15] T. J. Burns and E. S. Swanson, Phys. Lett. B, 760: 627 (2016)
    [16] L. Tang and C. F. Qiao, Eur. Phys. J. C, 76: 558 (2016)
    [17] F. K. Guo, U. G. Meissner and B. S. Zou, Commun. Theor. Phys., 65: 593 (2016)
    [18] M. Albaladejo, J. Nieves, E. Oset, Z. F. Sun and X. Liu, Phys. Lett. B, 757: 515 (2016)
    [19] A. Esposito, A. Pilloni and A. D. Polosa, Phys. Lett. B, 758:292 (2016)
    [20] J. X. Lu, X. L. Ren and L. S. Geng, Eur. Phys. J. C, 77: 94 (2017)
    [21] F. Goerke, T. Gutsche, M. A. Ivanov, J. G. Korner, V. E. Lyubovitskij and P. Santorelli, Phys. Rev. D, 94: 094017 (2016)
    [22] S. S. Agaev, K. Azizi, B. Barsbay and H. Sundu, Eur. Phys. J. A, 53: 11 (2017)
    [23] C. M. Zanetti, M. Nielsen and K. P. Khemchandani, Phys. Rev. D, 93: 096011 (2016)
    [24] Y. Jin and S. Y. Li, Phys. Rev. D, 94: 014023 (2016)
    [25] Q. F. Lu and Y. B. Dong, Phys. Rev. D, 94: 094041 (2016)
    [26] R. Albuquerque, S. Narison, A. Rabemananjara and D. Ra- betiarivony, Int. J. Mod. Phys. A, 31: 1650093 (2016)
    [27] X. Chen and J. Ping, Eur. Phys. J. C, 76: 351 (2016)
    [28] X. W. Kang and J. A. Oller, Phys. Rev. D, 94: 054010 (2016)
    [29] C. B. Lang, D. Mohler and S. Prelovsek, Phys. Rev. D, 94:074509 (2016)
    [30] R. Chen and X. Liu, Phys. Rev. D, 94: 034006 (2016)
    [31] R. Aaij et al (LHCb Collaboration), Phys. Rev. Lett., 117:152003 (2016)
    [32] CMS Collaboration [CMS Collaboration], CMS-PAS-BPH-16-002
    [33] F. K. Guo, C. Hanhart, S. Krewald and U. G. Meissner, Phys. Lett. B, 666: 251 (2008)
    [34] M. Altenbuchinger, L.-S. Geng and W. Weise, Phys. Rev. D,89: 014026 (2014)
    [35] L. Liu, K. Orginos, F. -K. Guo, C. Hanhart and U. -G. Meiss- ner, Phys. Rev. D, 87: 014508 (2013)
    [36] J. A. Oller and U. G. Meissner, Phys. Lett. B, 500: 263 (2001)
    [37] E. Oset and A. Ramos, Eur. Phys. J. A, 44: 445 (2010)
    [38] E. Oset and A. Ramos, Nucl. Phys. A, 635: 99 (1998)
    [39] D. Jido, J. A. Oller, E. Oset, A. Ramos and U. G. Meissner, Nucl. Phys. A, 725: 181 (2003)
    [40] R. Molina, D. Nicmorus and E. Oset, Phys. Rev. D, 78: 114018 (2008)
    [41] L. Geng and E. Oset, Phys. Rev. D, 79: 074009 (2009)
    [42] S. Sarkar, B. X. Sun, E. Oset and M. J. Vicente Vacas, Eur. Phys. J. A, 44: 431 (2010)
    [43] L. M. Abreu, D. Cabrera, F. J. Llanes-Estrada and J. M. Torres-Rincon, Annals Phys., 326: 2737 (2011)
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Bao-Xi Sun, Fang-Yong Dong and Jing-Long Pang. Study of X(5568) in a unitary coupled-channel approximationof BK and B sπ[J]. Chinese Physics C, 2017, 41(7): 074104. doi: 10.1088/1674-1137/41/7/074104
Bao-Xi Sun, Fang-Yong Dong and Jing-Long Pang. Study of X(5568) in a unitary coupled-channel approximationof BK and B sπ[J]. Chinese Physics C, 2017, 41(7): 074104. doi:10.1088/1674-1137/41/7/074104 shu
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Received: 2017-01-04
Revised: 2017-03-05
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    Study ofX(5568) in a unitary coupled-channel approximationof BK and Bsπ

      Corresponding author:Bao-Xi Sun,
    • 1. College of Applied Sciences, Beijing University of Technology, Beijing 100124, China
    • 2. Department of Physics, Peking University, Beijing 100871, China
    • 3. College of Applied Sciences, Beijing University of Technology, Beijing 100124, China
    • 4. Department of Physics, Peking University, Beijing 100871, China

      Abstract:The potential of the m B meson and the pseudoscalar meson is constructed up to the next-to-leading order Lagrangian, and then the m BKand m Bsπ interaction is studied in the unitary coupled-channel approximation. A resonant state with a mass about 5568 MeV andJP=0+is generated dynamically, which can be associated with theX(5568) state announced by the D0 Collaboration recently. The mass and the decay width of this resonant state depend on the regularization scale in the dimensional regularization scheme, or the maximum momentum in the momentum cutoff regularization scheme. The scattering amplitude of the vectorBmeson and the pseudoscalar meson is calculated, and an axial-vector state with a mass near 5620 MeV andJP=1+is produced. Their partners in the charm sector are also discussed.

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