Erratum and Addendum: Analytical formula for the cross section of hadron 2 production from e+e collisions around the narrow charmouinum resonances (Chin. Phys. C, 48(11): 113104 (2024))

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Yanan Wang, Yadi Wang and Ping Wang. Erratum and Addendum: Analytical formula for the cross section of hadron 2 production from e+e collisions around the narrow charmouinum resonances (Chin. Phys. C, 48(11): 113104 (2024))[J]. Chinese Physics C. doi: 10.1088/1674-1137/adb709
Yanan Wang, Yadi Wang and Ping Wang. Erratum and Addendum: Analytical formula for the cross section of hadron 2 production from e+e collisions around the narrow charmouinum resonances (Chin. Phys. C, 48(11): 113104 (2024))[J]. Chinese Physics C.  doi: 10.1088/1674-1137/adb709 shu
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Received: 2025-02-17
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Erratum and Addendum: Analytical formula for the cross section of hadron 2 production from e+e collisions around the narrow charmouinum resonances (Chin. Phys. C, 48(11): 113104 (2024))

  • 1. North China Electric Power Unversity, Beijing 102206, China
  • 2. Institute of High Energy Physics, Chinese Academy of Sciences, Beijing 100049, China

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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 pubshlied 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.

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