中文

硬壁全息 QCD 中的粲介子耦合

高能物理 - 唯象学 2021-02-24 v2

摘要

我们研究四味硬壁全息 QCD,以评估 (D(),Dˉ0,a1)(D^{-(*-)}, \bar{D}^{0}, a_1^{-})(D(),Dˉ0,b1)(D^{-(*-)}, \bar{D}^{0}, b_1^{-})(Ds(),Dˉ0,K1A)(D_{s}^{-(*-)},\bar{D}^{0}, K_{1A}^{-})(Ds(),Dˉ0,K1B())(D_s^{-(*-)}, \bar{D}^{0}, K_{1B}^{-(*-)})(Ds+(+),D+,K1A0)(D_s^{+(*+)}, D^{+}, K_{1A}^{0})(Ds+(+),D+,K1B0)(D_s^{+(*+)}, D^{+}, K_{1B}^{0})(D(),Dˉ0(0),ρ)(D^{-(*-)}, \bar{D}^{0(*0)}, \rho^{-})(Ds(),Dˉ0(0),K)(D_s^{-(*-)}, \bar{D}^{0(*0)}, K^{*-})(D0(0),Dˉ0(0),ψ)(D^{0(*0)}, \bar{D}^{0(*0)}, \psi)(D1,Dˉ10,π)(D_1^{-}, \bar{D}_1^{0}, \pi^{-})(Ds1,Dˉ10,K)(D_{s1}^{-}, \bar{D}_1^{0}, K^{-})(D10,Dˉ10,ηc)(D_1^{0}, \bar{D}_1^{0}, \eta_c)(ψ,D0(0),D+,π)(\psi, D^{0(*0)}, D^{+}, \pi^{-})(ψ,D0(0),Dˉ0,π0)(\psi, D^{0(*0)}, \bar{D}^{0}, \pi^{0})(ψ,Ds+(+),D,K0)(\psi, D_{s}^{+(*+)}, D^{-}, K^{0})(ψ,D0(0),D+,a1)(\psi, D^{0(*0)}, D^{+}, a_1^{-})(ψ,D0(0),D+,b1)(\psi, D^{0(*0)}, D^{+}, b_1^{-})(ψ,Ds+(+),D,K1B0)(\psi, D_s^{+(*+)}, D^{-}, K_{1B}^{0})(ψ,Ds+(+),D,K1B0)(\psi, D_s^{+(*+)}, D^{-}, K_{1B}^{0}) 顶点的耦合。此外,本研究还估算了 D0(0)D^{0(*0)}Ds()D_s^{-(*-)}ω\omegaψ\psiD10D_1^{0}D1D_1^{-}K0K^0ηc\eta_{c}Ds1D_{s1}^{-}χc1\chi_{c1} 的质量以及 π\pi^-D()D^{-(*-)}KK^-ρ\rho^-D1D_1^{-}a1a_1^-Ds()D_s^{-(*-)} 的衰变常数。我们还将所得结果与质量和衰变常数的实验值进行了比较。我们的强耦合结果也与 3PSR 和 LCSR 预言进行了比较。

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引用

@article{arxiv.2007.02273,
  title  = {Charm meson couplings in hard-wall Holographic QCD},
  author = {S. Momeni and M. Saghebfar},
  journal= {arXiv preprint arXiv:2007.02273},
  year   = {2021}
}