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2024年10月30日

Low-lying 1/2- hidden strange pentaquark states in the constituent quark model

  • We investigate the spectrum of the low-lying 1/2- hidden strange pentaquark states, employing the constituent quark model, and looking at two ways within that model of mediating the hyperfine interaction between quarks-Goldstone boson exchange and one gluon exchange. Numerical results show that the lowest 1/2- hidden strange pentaquark state in the Goldstone boson exchange model lies at~1570 MeV, so this pentaquark configuration may form a notable component in S11(1535) if the Goldstone boson exchange model is applied. This is consistent with the prediction that S11(1535) couples very strongly to strangeness channels.
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  • [1] R. Aaij et al (LHCb Collaboration), Phys. Rev. Lett., 115:072001(2015)
    [2] M. Karliner and J. L. Rosner, Phys. Rev. Lett., 115:122001(2015)
    [3] R. Chen, X. Liu, X. Q. Li et al, Phys. Rev. Lett., 115:132002(2015)
    [4] H. X. Chen, W. Chen, X. Liu et al, Phys. Rev. Lett., 115:172001(2015)
    [5] L. Roca, J. Nieves, and E. Oset, Phys. Rev. D, 92:094003(2015)
    [6] J. He, Phys. Lett. B, 753:547(2016)
    [7] F. K. Guo, U. G. Meissner, W. Wang et al, Phys. Rev. D, 92:071502(2015)
    [8] H. X. Chen, W. Chen, X. Liu et al, Phys. Rept., 639:1(2016)
    [9] F. K. Guo, C. Hanhart, U. G. Meissner et al, arXiv:1705.00141
    [10] J. J. Wu, R. Molina, E. Oset et al, Phys. Rev. Lett., 105:232001(2010)
    [11] S. G. Yuan, K. W. Wei, J. He et al, Eur. Phys. J. A, 48:61(2012)
    [12] H. Gao, H. Huang, T. Liu et al, Phys. Rev. C, 95:055202(2017)
    [13] C. Patrignani et al (Particle Data Group), Chin. Phys. C, 40:100001(2016)
    [14] B. C. Liu and B. S. Zou, Phys. Rev. Lett., 96:042002(2006)
    [15] J. J. Xie, B. S. Zou, and H. C. Chiang, Phys. Rev. C, 77:015206(2008)
    [16] N. Isgur and G. Karl, Phys. Rev. D, 18:4187(1978)
    [17] S. Capstick and W. Roberts, Prog. Part. Nucl. Phys., 45:S241(2000)
    [18] L. Y. Glozman and D. O. Riska, Phys. Rept., 268:263(1996)
    [19] N. Kaiser, P. B. Siegel, and W. Weise, Phys. Lett. B, 362:23(1995)
    [20] T. Inoue, E. Oset, and M. J. Vicente Vacas, Phys. Rev. C, 65:035204(2002)
    [21] P. C. Bruns, M. Mai, and U. G. Meissner, Phys. Lett. B, 697:254(2011)
    [22] B. S. Zou and D. O. Riska, Phys. Rev. Lett., 95:072001(2005)
    [23] C. S. An, D. O. Riska, and B. S. Zou, Phys. Rev. C, 73:035207(2006)
    [24] D. O. Riska and B. S. Zou, Phys. Lett. B, 636:265(2006)
    [25] R. Bijker and E. Santopinto, Phys. Rev. C, 80:065210(2009)
    [26] R. Bijker, J. Ferretti, and E. Santopinto, Phys. Rev. C, 85:035204(2012).
    [27] C. S. An and B. S. Zou, Eur. Phys. J. A, 39:195(2009)
    [28] C. S. An and B. S. Zou, Sci. Sin. G, 52:1452(2009)
    [29] C. An and B. Saghai, Phys. Rev. C, 84:045204(2011)
    [30] B. Saghai and Z. p. Li, Eur. Phys. J. A, 11:217(2001)
    [31] S. G. Yuan, C. S. An, K. W. Wei et al, Phys. Rev. C, 87:025205(2013)
    [32] C. S. An and H. Chen, Phys. Rev. D, 96:034012(2017)
    [33] C. S. An and D. O. Riska, Eur. Phys. J. A, 37:263(2008)
    [34] L. Y. Glozman and D. O. Riska, Nucl. Phys. A, 603:326(1996)[Erratum-ibid. A, 620:510(1997)]
    [35] J. Leandri and B. Silvestre-Brac, Phys. Rev. D, 40:2340(1989)
    [36] B. Silvestre-Brac, and J. Leandri, Phys. Rev. D, 45:4221(1992)
    [37] F. Buccella, H. Hogaasen, J. -M. Richard et al, Eur. Phys. J. C, 49:743(2007)
    [38] H. Hogaasen, J. M. Richard, and P. Sorba, Phys. Rev. D, 73:054013(2006)
    [39] C. Helminen and D. O. Riska, Nucl. Phys. A, 699:624(2002)
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Get Citation
Hui Li, Zong-Xiu Wu, Chun-Sheng An and Hong Chen. Low-lying 1/2- hidden strange pentaquark states in the constituent quark model[J]. Chinese Physics C, 2017, 41(12): 124104. doi: 10.1088/1674-1137/41/12/124104
Hui Li, Zong-Xiu Wu, Chun-Sheng An and Hong Chen. Low-lying 1/2- hidden strange pentaquark states in the constituent quark model[J]. Chinese Physics C, 2017, 41(12): 124104.  doi: 10.1088/1674-1137/41/12/124104 shu
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Received: 2017-09-02
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    Supported by National Natural Science Foundation of China (11675131, 11645002), Chongqing Natural Science Foundation (cstc2015jcyjA00032) and Fundamental Research Funds for the Central Universities (SWU115020)

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Low-lying 1/2- hidden strange pentaquark states in the constituent quark model

    Corresponding author: Chun-Sheng An,
  • 1. School of Physical Science and Technology, Southwest University, Chongqing 400715, China
Fund Project:  Supported by National Natural Science Foundation of China (11675131, 11645002), Chongqing Natural Science Foundation (cstc2015jcyjA00032) and Fundamental Research Funds for the Central Universities (SWU115020)

Abstract: We investigate the spectrum of the low-lying 1/2- hidden strange pentaquark states, employing the constituent quark model, and looking at two ways within that model of mediating the hyperfine interaction between quarks-Goldstone boson exchange and one gluon exchange. Numerical results show that the lowest 1/2- hidden strange pentaquark state in the Goldstone boson exchange model lies at~1570 MeV, so this pentaquark configuration may form a notable component in S11(1535) if the Goldstone boson exchange model is applied. This is consistent with the prediction that S11(1535) couples very strongly to strangeness channels.

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