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基于分子态构型研究单粲味五夸克态的产生

邢晔 李娜 杨翎彬 胡晓会

邢晔, 李娜, 杨翎彬, 胡晓会. 基于分子态构型研究单粲味五夸克态的产生. 物理学报, 2024, 73(13): 131401. doi: 10.7498/aps.73.20240447
引用本文: 邢晔, 李娜, 杨翎彬, 胡晓会. 基于分子态构型研究单粲味五夸克态的产生. 物理学报, 2024, 73(13): 131401. doi: 10.7498/aps.73.20240447
Xing Ye, Li Na, Yang Ling-Bin, Hu Xiao-Hui. Production of single charm pentaquark based on molecular configuration. Acta Phys. Sin., 2024, 73(13): 131401. doi: 10.7498/aps.73.20240447
Citation: Xing Ye, Li Na, Yang Ling-Bin, Hu Xiao-Hui. Production of single charm pentaquark based on molecular configuration. Acta Phys. Sin., 2024, 73(13): 131401. doi: 10.7498/aps.73.20240447

基于分子态构型研究单粲味五夸克态的产生

邢晔, 李娜, 杨翎彬, 胡晓会

Production of single charm pentaquark based on molecular configuration

Xing Ye, Li Na, Yang Ling-Bin, Hu Xiao-Hui
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  • 基于有效拉氏量方法, 本文研究了自旋宇称为JP=1/2的单粲味五夸克态的产生. 本文根据强子可能的分子态图像, 分别以NDsNDs不同的分子态构型, 讨论了Bs介子产生单粲味五夸克态cˉsuud和十重态重子ˉΔ, 以及该五夸克态的两体强衰变过程. 通过复合粒子判据, 计算出与单粲味五夸克态cˉsuud相关的强耦合常数. 借助于强子的有效拉氏量方法, 最终得到了单粲味五夸克态的产生分支比. 结果表明, 在单粲味五夸克态cˉsuudNDs的构型下, 具有Cabibbo允许的产生过程: ˉBsPcˉsˉΔ的分支比可以达到105量级, 而在NDs的构型下, 该过程的分支比仅为108量级. 本文的研究结果可以为单粲味五夸克态的实验搜寻和深入研究提供参考, 并期望在将来的实验探测诸如LHCb, Belle II, BaBar等B工厂中得到验证.
    In this work, the authors use the effective Lagrangian method to investigate the production of singly charm pentaquark state with spin parity JP=1/2. Based on the possible molecular state images of hadrons, the author discusses the production of singly charm pentaquark state cˉsuud and decuplet baryon ˉΔ by Bs meson with different molecular state configurations of NDs or NDs. To determine the coupling between pentaquark and their constituents in the molecular scheme, the authors follow the Weinberg compositeness condition to estimate the self-energy diagram of the singly charmed pentaquark. Further study on the production of pentaquark from Bs meson can be propeled by computing the transition matrix elements, or the triangle diagrams, which can be careful divided into two part subprocess, one associated with weak transition can be represented into form factor and decay constant, another one related to strong coupling of hadrons can be described by effective Lagrangian. Selecting the scale parameter α (10–200 MeV) and binding energy ε (5, 20, 50 MeV), the authors can find the branching ratio of the production ˉBsPcˉsˉΔ. Under the configuration of NDs molecule, the branching ratio of the Cabibbo allowed process ˉBsPcˉsˉΔ can reach to order of 105. Moreover, the production branching ratio of NDs molecule is only at the order of 108. A increasing scale parameter α can significantly improve the production branching ratio of the singly charm pentaquark. In addition, the binding energy and the coupling constants will also affect the magnitude of production. Therefore, considering the above factors, the production branching ratio of singly charm pentaquark in Bs decays have considerable results, which is worth experimental and theoretical research in the future. The findings of our work can provide a reference for the experimental search and study of singly charm pentaquark, and it is hoped that they will be verified in future experimental detections at B factories such as LHCb, Belle, and BaBar.
      通信作者: 李娜, TS22180005A31@cumt.edu.cn
    • 基金项目: 国家自然科学基金(批准号: 12005294)资助的课题.
      Corresponding author: Li Na, TS22180005A31@cumt.edu.cn
    • Funds: Project supported by the National Natural Science Foundation of China (Grant No. 12005294).
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    Aaij R, Abellán Beteta C, Adeva B, et al. 2019 Phys. Rev. Lett. 122 222001Google Scholar

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    Azizi K, Sarac Y, Sundu H 2023 Phys. Rev. D 107 014023Google Scholar

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    Chen R, Liu X, Li X Q, Zhu S L 2015 Phys. Rev. Lett. 115 132002Google Scholar

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    Guo F K, Meißner Ulf-G, Wang W, Yang Z 2015 Phys. Rev. D 92 071502Google Scholar

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    Branz T, Gutsche T, Lyubovitskij V E 2021 Phys. Rev. D 104 114028Google Scholar

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    Zhang Y, He G Z, Ye Q X, Y D C, Hua J, Wang Q 2024 Chin. Phys. Lett. 41 021301Google Scholar

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    Chen H X, Chen W Z, Shi L 2019 Phys. Rev. D 100 051501Google Scholar

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    Liu M Z, Pan Y W, Peng F Z, Sánchez Sánchez M, Geng L S, Hosaka A, Pavon V M 2019 Phys. Rev. Lett. 122 242001Google Scholar

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    Zhu J T, Kong S Y, He J 2023 Am. Phys. Soc. 107 034029Google Scholar

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    Peng F Z, Yan M J, Sánchez Sánchez M, Valderrama M P 2021 Eur. Phys. J. C 81 666Google Scholar

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    叶全兴, 何广朝, 王倩 2023 物理学报 72 201401Google Scholar

    Ye Q X, He G C, Wang Q 2023 Acta Phys. Sin. 72 201401Google Scholar

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    Shi P P, Baru Vadim, Guo F K, Hanhart C, Nefediev A 2024 Chin. Phys. Lett. 41 031301Google Scholar

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    Li N, Xing Y, Hu X H 2023 Eur. Phys. J. C 83 1013Google Scholar

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    Huang Y, Xiao C J, Lü Q F, Wang R, He J, Geng L S 2018 Phys. Rev. D 97 094013Google Scholar

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    Zhu H Q, Ma N N, Huang Y 2020 Eur. Phys. J. C 80 1184Google Scholar

    [26]

    Yan Y, Hu X H, Huang H X, Ping J L 2023 Phys. Rev. D 108 094045Google Scholar

    [27]

    Xin Q, Yang X, Wang Z G 2023 Int. J. Mod. Phys. A 38 2350123Google Scholar

    [28]

    Yan M J, Peng F Z, Pavon V M 2024 Phys. Rev. D 109 014023Google Scholar

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    McLean E, Davies C T H, Koponen J, Lytle A T 2020 Phys. Rev. D 101 074513Google Scholar

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    Heng H Y 1997 Phys. Rev. D 56 2799Google Scholar

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    Thomas G, Mikhail A I, Jürgen G K, et al. 2015 Phys. Rev. D 91 074001Google Scholar

    [38]

    Wu S M, Wang F, Zou B S 2023 Phys. Rev. C 108 045201Google Scholar

    [39]

    Li H N, Lu C D, Yu F S 2012 Phys. Rev. D 86 036012Google Scholar

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    Xing Y, Xing Z P 2019 Chin. Phys. C 43 073103Google Scholar

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    Xu Y J, Cui C Y, Liu Y L, Huang M Q 2020 Phys. Rev. D 102 034028Google Scholar

  • 图 1  具有ND()s分子态构型的单粲味五夸克态的自能图

    Fig. 1.  Self-energy diagram of singly charm pentaquark as hadronic molecules ND()s.

    图 2  ˉBs介子产生单粲五夸克的三角图 (a), (b)具有NDs分子态构型的单粲五夸克; (c), (d) 具有NDs分子态构型的单粲五夸克

    Fig. 2.  Triangle diagrams of singly charm pentaquark produced by ˉBs meson: (a), (b) Singly charm pentaquark with NDs molecular state configuration; (c), (d) singly charm pentaquark with NDs molecular state configuration.

    图 3  ˉBs介子弱衰变过程的W发射图

    Fig. 3.  W emission diagram of ˉBs meson weak decay

    图 4  ˉBsNPcˉsˉΔ的分支比随参数α的变化曲线 (a) PcˉsNDs分子态; (b) PcˉsNDs分子态

    Fig. 4.  Branching ratios of ˉBsNPcˉsˉΔ vary with the parameter α: (a) Pcˉs as hadronic molecule NDs; (b) Pcˉs as hadronic molecule NDs

    表 1  形状因子F1(k2), F2(k2)Ai(k2)(i = 1, 2, 3)的拟合展开参数aimpole[34,35]

    Table 1.  Fitted parameters ai and pole mass mpole of form factors F1(k2), F2(k2) and Ai(k2)(i = 1, 2, 3)[34,35].

    参数 ˉBsD ˉBsD
    F1(k1) F2(k1) A0(k1) A1(k1) A2(k1) A3(k1)
    a0 0.666 0.666 0.100 0.105 0.055 0.059
    a1 0.206 3.236 0.180 0.430 0.010 0.110
    a2 0.106 0.075 0.006 0.100 0.030 0.250
    a3 0.00 0.00 0.00 0.030 0.060 0.050
    mpole/GeV 6.335 6.275 6.745 6.745
    下载: 导出CSV

    表 2  单粲味五夸克态的产生分支比(α = 100 MeV)

    Table 2.  Production branching ratio of singly charm pentaquark state (α = 100 MeV).

    分子态 产生道 分支比(×106)
    ε/MeV
    5 20 50
    NDs ˉBsNPcˉsˉΔ 29.40 31.37 24.51
    ˉBsNPcˉs(ΛcK)ˉΔ 0.223 0.194 0.137
    NDs ˉBsNPcˉsˉΔ 0.055 0.408 1.570
    ˉBsNPcˉs(ΛcK)ˉΔ 0.0006 0.0041 0.0157
    ˉBsNPcˉs(ΣcK)ˉΔ 0.0004 0.0024 0.0072
    ˉBsNPcˉs(pDs)ˉΔ 0.0002 0.0015 0.0050
    下载: 导出CSV
  • [1]

    Aaij R, Advea B, Adinolfi M, et al. 2015 Phys. Rev. Lett. 115 072001Google Scholar

    [2]

    Aaij R, Abellán Beteta C, Adeva B, et al. 2019 Phys. Rev. Lett. 122 222001Google Scholar

    [3]

    Aaij R, Abellán Beteta C, Ackernley T, et al. 2021 Sci. Bull. 66 1278Google Scholar

    [4]

    Aaij R, Abdelmotteleb A S W, Abellán Beteta C, et al. 2022 Phys. Rev. Lett. 128 062001Google Scholar

    [5]

    Santopinto E, Giachino A 2017 Phys. Rev. D 96 014014Google Scholar

    [6]

    Deng C R, Ping J L, Huang H X, Wang F 2017 Phys. Rev. D 95 014031Google Scholar

    [7]

    Azizi K, Sarac Y, Sundu H 2023 Phys. Rev. D 107 014023Google Scholar

    [8]

    Chen R, Liu X, Li X Q, Zhu S L 2015 Phys. Rev. Lett. 115 132002Google Scholar

    [9]

    Guo F K, Meißner Ulf-G, Wang W, Yang Z 2015 Phys. Rev. D 92 071502Google Scholar

    [10]

    Branz T, Gutsche T, Lyubovitskij V E 2021 Phys. Rev. D 104 114028Google Scholar

    [11]

    Lebed R F, Martinez S R 2022 Phys. Rev. D 106 074007Google Scholar

    [12]

    Zhang Y, He G Z, Ye Q X, Y D C, Hua J, Wang Q 2024 Chin. Phys. Lett. 41 021301Google Scholar

    [13]

    Chen H X, Chen W Z, Shi L 2019 Phys. Rev. D 100 051501Google Scholar

    [14]

    Liu M Z, Pan Y W, Peng F Z, Sánchez Sánchez M, Geng L S, Hosaka A, Pavon V M 2019 Phys. Rev. Lett. 122 242001Google Scholar

    [15]

    Zhu J T, Kong S Y, He J 2023 Am. Phys. Soc. 107 034029Google Scholar

    [16]

    Wu Q, Chen D Y 2019 Phys. Rev. D 100 114002Google Scholar

    [17]

    Peng F Z, Yan M J, Sánchez Sánchez M, Valderrama M P 2021 Eur. Phys. J. C 81 666Google Scholar

    [18]

    Xiao C W, Wu J J, Zou B S 2021 Phys. Rev. D 103 054016Google Scholar

    [19]

    Lu J X, Liu M Z, Shi R X, Geng L S 2021 Phys. Rev. D 104 034022Google Scholar

    [20]

    Wu Q, Chen D Y, Ji R 2021 Chin. Phys. Lett. 38 071301Google Scholar

    [21]

    叶全兴, 何广朝, 王倩 2023 物理学报 72 201401Google Scholar

    Ye Q X, He G C, Wang Q 2023 Acta Phys. Sin. 72 201401Google Scholar

    [22]

    Shi P P, Baru Vadim, Guo F K, Hanhart C, Nefediev A 2024 Chin. Phys. Lett. 41 031301Google Scholar

    [23]

    Li N, Xing Y, Hu X H 2023 Eur. Phys. J. C 83 1013Google Scholar

    [24]

    Huang Y, Xiao C J, Lü Q F, Wang R, He J, Geng L S 2018 Phys. Rev. D 97 094013Google Scholar

    [25]

    Zhu H Q, Ma N N, Huang Y 2020 Eur. Phys. J. C 80 1184Google Scholar

    [26]

    Yan Y, Hu X H, Huang H X, Ping J L 2023 Phys. Rev. D 108 094045Google Scholar

    [27]

    Xin Q, Yang X, Wang Z G 2023 Int. J. Mod. Phys. A 38 2350123Google Scholar

    [28]

    Yan M J, Peng F Z, Pavon V M 2024 Phys. Rev. D 109 014023Google Scholar

    [29]

    Steven W 1963 Phys. Rev. 130 776Google Scholar

    [30]

    Tanja B, Thomas G, Valery E L 2009 Phys. Rev. D 79 014035Google Scholar

    [31]

    Xiao C J, Huang Y, Dong Y B, Geng L S, Chen D Y 2019 Phys. Rev. D 100 014022Google Scholar

    [32]

    Shen C W, Wu J J, Zou B S 2019 Phys. Rev. D 100 056006Google Scholar

    [33]

    Yalikun N, Zou B S 2022 Phys. Rev. D 105 094026Google Scholar

    [34]

    McLean E, Davies C T H, Koponen J, Lytle A T 2020 Phys. Rev. D 101 074513Google Scholar

    [35]

    Harrison J D, Christine T H 2022 Phys. Rev. D 105 094506Google Scholar

    [36]

    Heng H Y 1997 Phys. Rev. D 56 2799Google Scholar

    [37]

    Thomas G, Mikhail A I, Jürgen G K, et al. 2015 Phys. Rev. D 91 074001Google Scholar

    [38]

    Wu S M, Wang F, Zou B S 2023 Phys. Rev. C 108 045201Google Scholar

    [39]

    Li H N, Lu C D, Yu F S 2012 Phys. Rev. D 86 036012Google Scholar

    [40]

    Xing Y, Xing Z P 2019 Chin. Phys. C 43 073103Google Scholar

    [41]

    Xu Y J, Cui C Y, Liu Y L, Huang M Q 2020 Phys. Rev. D 102 034028Google Scholar

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  • 收稿日期:  2024-03-30
  • 修回日期:  2024-05-11
  • 上网日期:  2024-05-21
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