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This paper was published online on 8 August 2024 with a typo sign in Eq. (3), plots in Fig. 5 being mistaken, and the acknowledgement of an author being missed. The function
$F(x, s)$ in Eq. (3) in the published version of the journal should be corrected as:$ \begin{aligned}[b] F(x, s)=\;&t x^{t-1}(1+\delta)-t(1-\frac{x}{2}) \\ + &\frac{t^2}{8}\left[4(2-x)\ln\frac{1}{x}-\frac{1+3(1-x)^2}{x}\ln(1-x) -6+x\right]. \end{aligned} $
(1) The parameters have the same meaning with those in the published version. The other formulas or conclusions remain unaffected. The plots for the comparison with
$n=2$ for a bayron pair in Fig. 5 in publied version are corrected as Fig. 1 in this erratum.
Figure 1. (color online) Difference between DTFI and AAF with
$n=2$ in different assumptions of$\mathcal{C}$ ,$\mathcal{F}$ and$\Phi$ . The color in each box stands for the largest differnce between$3.67$ GeV to$3.70$ GeV.
Erratum and Addendum: Analytical formula for the cross section of hadron production from e+e− collisions around the narrow charmouinum resonances (Chin. Phys. C, 48(11): 113104 (2024))
- Received Date: 2025-02-17
- Available Online: 2025-03-15
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