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Abstract
This erratum corrects a typographical error in Eq. (4) of our published paper [Opt. Express 30(18), 31584 (2022). [CrossRef] ]. This misprint does not influence the results and conclusions presented in the original Article.
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There is a typographical error in Eq. (4) of our published paper [1]. The correct form of Eq. (4) should be:
$$\begin{aligned} {Q_{tot}}({{\theta_2},{\theta_3}} )&= {Q_{12}}({{\theta_2},{\theta_3}} )+ {Q_{13}}({{\theta_2},{\theta_3}} )\\ &= \int_{ - \infty }^\infty {\frac{{d\beta }}{{2\pi }}|\beta |} \int_0^\infty {\frac{{d\omega }}{{2\pi }}} \int_0^\pi {\frac{{d\phi }}{{2\pi }}} [{{\Theta _{12}}({\omega ,T,\Delta {T_1}} ){\xi^{({1,2} )}}({\omega ,\beta ,\phi ,{\theta_2},{\theta_3}} )} \\ &{ + \textrm{ }{\Theta _{13}}({\omega ,T,\Delta {T_1},\Delta {T_2}} ){\xi^{({1,3} )}}({\omega ,\beta ,\phi ,{\theta_2},{\theta_3}} )} ], \end{aligned}$$
the differences being removing the summation of s and p polarizations as this has been included by the trace formula, replacing the upper limit of the integral with respect to $\omega $ from $\pi $ to $\infty $, adding the third integral with respect to the incident angle $\phi $, and correcting the photon transmission coefficient ${\Theta _{13}}$ from ${\Theta _{13}}({\omega ,T,\Delta {T_2}} )$ to ${\Theta _{13}}({\omega ,T,\Delta {T_1},\Delta {T_2}} )$ such that the dependence on the temperature of the body 1 $T + \Delta {T_1}$ can be explicitly reflected. The numerical calculations in the original Article were performed using the correct equation and this correction has no impact on the presented results and the conclusions of the original Article.Disclosures
The authors declare that there are no conflicts of interest related to this article.
References
1. Z. Yu, X. Li, T. Lee, and H. Iizuka, “Near-field radiative heat transfer in three-body Weyl semimetals,” Opt. Express 30(18), 31584 (2022). [CrossRef]