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Root mean square radii of heavy flavoured mesons in a quantum chromodynamics potential model

机译:量子色动力学势模型中重味介子的均方根半径

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We report the results of root mean square (r.m.s.) radii of heavy flavoured mesons in a QCD model with the potential $V (r) = a?’(4alpha_{s}/3r) + br + c$. As the potential is not analytically solvable, we first obtain the results in the absence of confinement and Coulomb terms respectively. Confinement and Coulomb effects are then introduced successively in the approach using the Dalgarnoa€?s method of perturbation. We explicitly consider the following two quantum mechanical aspects in the analysis: (a) The scale factor $c$ in the potential should not effect the wave function of the system even while applying the perturbation theory. (b) Choice of perturbative piece of the Hamiltonian (confinement or linear) should determine the effective radial separation between the quarks and antiquarks. The results are then compared with the available theoretical values of r.m.s. radii.
机译:我们报告了QCD模型中重味介子的均方根(r.m.s.)半径,其结果可能是$ V(r)= a?’(4alpha_ {s} / 3r)+ br + c $。由于电位无法解析解决,因此我们首先分别在没有限制和库仑项的情况下获得结果。然后,采用达加诺亚(Dalgarnoa)的摄动法在该方法中依次引入了约束和库仑效应。我们在分析中明确考虑了以下两个量子力学方面:(a)即使应用微扰理论,势中的比例因子$ c $也不应影响系统的波动函数。 (b)哈密顿量的扰动部分(约束或线性)的选择应确定夸克和反夸克之间的有效径向间隔。然后将结果与r.m.s的可用理论值进行比较。半径

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