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中国物理学会期刊

利用光锥求和规则方法计算强子耦合常数\calB_\rmcc\calB_\rmc^6 \rmD

CSTR: 32037.14.aps.75.20260295

Study on the strong coupling constants \calB_\rmcc\calB_\rmc^6\rmD using the light-cone sum rules method

CSTR: 32037.14.aps.75.20260295
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  • 自双粲重子发现以来, 大型强子对撞机持续探寻更多双重重子信号. 随着数据的不断积累, 未来有望观测到更多此类重子态, 相关理论研究对实验识别具有重要意义. 在双粲重子弱衰变过程, 尤其是非轻衰变中, 显著的末态相互作用常给理论计算带来较大不确定性. 利用末态相互作用方法研究粲-底重子非轻弱衰变时, 需要输入自旋为1/2的双粲重子和单粲重子与粲味介子之间的强耦合常数, 然而目前较为缺乏此类参数的理论研究. 为填补这一空白, 本文基于光锥量子色动力学求和规则, 从自旋为1/2的单粲味重子六重态\calB_\rmc^6的光锥分布振幅出发, 构建强子耦合常数g_\calB_\rmcc\calB_\rmc^6 \rmD的关联函数. 并分别计算强子层次与夸克层次的关联函数, 利用夸克-强子对偶, 推导出此类耦合常数求和规则的解析表达式, 并给出数值结果和误差分析. 本研究为双粲重子的强衰变与弱衰变动力学提供了关键的理论输入参数, 相关结果可直接用于相关衰变过程的理论研究.

     

    In this work, we systematically investigate the strong coupling constants for vertices involving doubly charmed baryons ( \calB_\rmcc), singly charmed sextet baryons ( \calB_\rmc^6), and D mesons, using the light-cone sum rules method. The calculations are performed analytically and numerically, with the non-perturbative input taken as the light-cone distribution amplitudes of the singly charmed baryon \calB_\rmc^6. Through graphical analysis, we determine the optimal Borel parameter ranges and present numerical results with a thorough error estimate, accounting for uncertainties in the Borel parameters, the continuum thresholds and the decay constants. To extrapolate the b-baryon light-cone distribution amplitudes to c-baryons, we adopt a simple scaling method, and the uncertainty from the scaling factor is incorporated to reflect this extrapolation. The uncertainties induced by the decay constants \rmf_\calB_\rmcc and \rmf_\calB_\rmc^6 dominate over those from other parameters, which can be attributed to the significant inherent uncertainties of these input parameters. The light-cone sum rules results deviate from the ratios predicted by SU(3) flavor symmetry, which are primarily due to the significant differences in the light-cone wave functions of baryons with different light quarks (u, d, s) in the light-cone sum rules calculation. Furthermore, these deviations can be well accounted for by the ratios of input parameters such as masses and decay constants. The results can be cross-checked by other approaches such as conventional quantum chromodynamics sum rules or lattice quantum chromodynamics. These strong coupling constants are key inputs for analyzing non-leptonic weak decays of doubly heavy baryons, particularly for evaluating final-state interactions in charmed-bottom baryon decays. Our findings thus provide both theoretical insights into the strong and weak decay dynamics of doubly heavy baryons and a practical tool for experimental hadronic analyses.

     

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