Download PDF $$ \mu_{0}^{A S}=\frac{16 e \hbar N_{0}}{3 \cdot 2^{1.5} \pi x(1-x) E_{A S}^{2}\left(m_{\mathrm{s}}\right)^{2.5}\left(k_{\mathrm{B}} T\right)^{0.5}} $$ $$ \mu_{0}^{A S}=\frac{16 e \hbar^{4} N_{0}}{3 \cdot 2^{1.5} \pi x(1-x) E_{A S}^{2}\left(m_{\mathrm{s}}\right)^{2.5}\left(k_{\mathrm{B}} T\right)^{0.5}} $$ 
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Correction | Open Access | 4 Dec 2025
Correction: Poorer is better: towards robust, high performance Mg2(Si,Sn) thermoelectric material by avoiding excess Mg (Energy Mater 2025; 10.20517/energymater.2025.51)
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0 Energy Mater. 2025, 5, 500154.
10.20517/energymater.2025.201 |
© The Author(s) 2025.
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Correction to Energy Mater. 2025, 5, 500134.
In the original publication the authors later recognized that a power was missing in equation (10) of the main text. To rectify this error, they issued the following correction:
On page 14, in equation (10), the reduced Planck constant
The original equation is:
The corrected equation is:
We apologize for any inconvenience caused and state that the correct equation was used in all calculations, and the scientific conclusions are not affected. The original article has been updated accordingly.
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Correction
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Correction: Poorer is better: towards robust, high performance Mg2(Si,Sn) thermoelectric material by avoiding excess Mg (Energy Mater 2025; 10.20517/energymater.2025.51)
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