\begin{document}$\Omega_{b}$\end{document} states represented by interpolating currents with a derivative and calculate the corresponding masses and pole residues using the QCD sum rule method. Because of the large uncertainties in our calculation compared with the small difference in the masses of the excited \begin{document}$\Omega_{b}$\end{document} states observed by the LHCb collaboration, it is necessary to study other properties of the P-wave \begin{document}$\Omega_{b}$\end{document} states represented by the interpolating currents investigated in the present work to gain a better understanding of the four excited \begin{document}$\Omega_{b}$\end{document} states observed by the LHCb collaboration."> <i>P</i>-wave Ω<sub><i>b</i></sub> states: masses and pole residues -
  • [1]

    R.Aaijet al. (LHCb Collaboration), Phys. Rev. Lett.118, 182001 (2017)

  • [2]

    R. Aaijet al. (LHCb Collaboration), Phys. Rev. Lett.124, 082002 (2020)

  • [3]

    S. S. Agaev, K. Azizi, and H. Sundu, Eur. Phys. Lett.118, 61001 (2017)

  • [4]

    M. Karliner and J. L. Rosner, Phys. Rev. D95, 114012 (2017)

  • [5]

    H. X. Chen, Q. Mao, W. Chenet al., Phys. Rev. D95, 094008 (2017)

  • [6]

    G. Yang and J. L. Ping, Phys. Rev. D97, 034023 (2018)

  • [7]

    K. L. Wang, L. Y. Xiao, X. H. Zhonget al., Phys. Rev. D95, 116010 (2017)

  • [8]

    W. Wang and R. L. Zhu, Phys. Rev. D96, 014024 (2017)

  • [9]

    H. Y. Cheng and C. W. Chiang, Phys. Rev. D95, 094018 (2017)

  • [10]

    M. Padmanath and N. Mathur, Phys. Rev. Lett.119, 042001 (2017)

  • [11]

    H. X. Huang, J. L. Ping, and F. Wang, Phys. Rev. D97, 034027 (2018)

  • [12]

    Z. G. Wang, Eur. Phys. J. C77, 325 (2017)

  • [13]

    Z. Zhao, D. D. Ye, and A. L. Zhang, Phys. Rev. D95, 114024 (2017)

  • [14]

    B. Chen and X. Liu, Phys. Rev. D96, 094015 (2017)

  • [15]

    S. S. Agaev, K. Azizi, and H. Sundu, Eur. Phys. J. C77, 395 (2017)

  • [16]

    C. S. An and H. Chen, Phys. Rev. D96, 034012 (2017)

  • [17]

    Z. G. Wang, X. N. Wei, and Z. H. Yan, Eur. Phys. J. C77, 832 (2017)

  • [18]

    Q. Mao, H. X. Chen, A. Hosakaet al., Phys. Rev. D96, 074021 (2017)

  • [19]

    W. Liang and Q. F. Lü, Eur. Phys. J. C80, 198 (2020)

  • [20]

    H. X. Chen, E. L. Cui, A. Hosakaet al., Eur. Phys. J. C80, 256 (2020)

  • [21]

    W. H. Liang and E. Oset, Phys. Rev. D101, 054033 (2020)

  • [22]

    Z. G. Wang, Int. J. Mod. Phys. A35, 2050043 (2020)

  • [23]

    L. Y. Xiao, K. L. Wang, M. S. Liuet al., Eur. Phys. J. C80, 279 (2020)

  • [24]

    H. Mutuk, Eur. Phys. J. A56, 146 (2020)

  • [25]

    H. M. Yang and H. X. Chen, Phys. Rev. D101, 114013 (2020)

  • [26]

    M. Karliner and J. L. Rosner, Phys. Rev. D102, 014027 (2020)

  • [27]

    K. Azizi, Y. Sarac, and H. Sundu, Phys. Rev. D102, 034007 (2020)

  • [28]

    L. Y. Xiao and X. H. Zhong, Phys. Rev. D102, 014009 (2020)

  • [29]

    K. L. Wang, L. Y. Xiao, and X. H. Zhong, Phys. Rev. D102, 034029 (2020)

  • [30]

    H. M. Yang, H. X. Chen, and Q. Mao, Phys. Rev. D102, 114009 (2020)

  • [31]

    H. M. Yang and H. X. Chen, Phys. Rev. D104, 034037 (2021)

  • [32]

    S. S. Agaev, K. Azizi, and H. Sundu, Eur. Phys. J. A57, 201 (2021)

  • [33]

    H. Q. Zhu, N. N. Ma, and Y. Huang, Eur. Phys. J. C80, 1184 (2020)

  • [34]

    H. J. Wang, Z. Y. Di, and Z. G. Wang, Commun. Theor. Phys.73, 035201 (2021)

  • [35]

    H. Q. Zhu and Y. Huang, Chin. Phys. C44, 083101 (2020)

  • [36]

    Z. G. Wang and H. J. Wang, Chin. Phys. C45, 013109 (2021)

  • [37]

    H. X. Chen, W. Chen, Q. Maoet al., Phys. Rev. D91, 054034 (2015)

  • [38]

    M. A. Shifman, A. I. Vainshtein, and V. I. Zakharov, Nucl. Phys. B147, 385 (1979)

  • [39]

    M. A. Shifman, A. I. Vainshtein, and V. I. Zakharov, Nucl. Phys. B147, 448 (1979)

  • [40]

    M. Tanabashiet al. (Particle Data Group), Phys. Rev. D98, 030001 (2018)

Baidu
map