首页> 外文期刊>Physics Letters, B. Nuclear Physics and High Energy Physics >Erratum to 'M(13c*)-M(Bc) splitting from nonrelativistic renormalization group'[Phys. Lett. B 593 (2004) 124]
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Erratum to 'M(13c*)-M(Bc) splitting from nonrelativistic renormalization group'[Phys. Lett. B 593 (2004) 124]

机译:对“从相对论重归一化组中分裂出来的M(13c *)-M(Bc)”进行勘误。来吧B 593(2004)124]

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After Eq. (20) the expression for the Coulomb binding energy should be g = —Clas2mr/(2n2). In Eqs. (20), (22) the overall factor 41,2 ..r is missed. This changes the numerical analysis of Section 4. The perturbative error reduces to 11 MeV. The uncertainty introducedmi In2 by the error of as(Mz) is reduced to +1.4 MeV. The nonperturbative effects scale with the heavy quark masses at least as 1/(mi m2mr).Thus, from the analysis of charmonium system we obtain 3 MeV for the typical size of the nonperturbative contribution to the HFSin 8,, and take 10 MeV as a conservative estimate of the corresponding uncertainty. The final numerical result for the splitting becomesM(8,*)— M(8,)= 48 ±15(th)±111(Sas). The corrected Figs. 1 and 2 are given below.
机译:等式之后(20)库仑结合能的表达式应为g = -Clas2mr /(2n2)。在等式中(20),(22)缺少总因数41,2 ..r。这改变了第4节的数值分析。微扰误差降至11 MeV。由in(Mz)的误差引入In2的不确定性降低至+1.4 MeV。夸克质量至少为1 /(mi m2mr)时,非扰动效应的标度呈比例关系。因此,通过对charm的分析,对于HFSin 8的非扰动贡献的典型大小,我们获得3 MeV,并以10 MeV作为对相应不确定性的保守估计。分割的最终数值结果变为M(8,*)-M(8,)= 48±15(th)±111(Sas)。校正后的图。 1和2如下。

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