\begin{document}$\left\langle 111 \right\rangle $\end{document} direction at temperatures below 1400 K. As the temperature increases, it makes rotations from one \begin{document}$ \left\langle 111 \right\rangle$\end{document}- to other \begin{document}$\left\langle 111 \right\rangle $\end{document}-directions. Thus migration of di-interstitial atoms with the first nearest neighbor configuration exhibits a change in mechanism from one-dimensional to three-dimensional migration, keeping the stable \begin{document}$\left\langle 111 \right\rangle $\end{document} configuration in the whole investigated temperature range. The migration of di-interstitial atoms with the second nearest neighbor configuration is one-dimensional along the \begin{document}$\left\langle 111 \right\rangle$\end{document} direction within a certain temperature range. When the temperature is above 600 K, the di-interstitial atoms will dissociate into two individual self-interstitial atoms and move independently. However, the migration of di-interstitial atoms with the third nearest neighbor configuration dissociates at a temperature just above 300 K. The non-parallel self-interstitial atoms form a sessile configuration within a certain temperature range. Once the sessile cluster is formed it can hardly move. Interestingly, it will transform into mobile defect when the temperature is higher than 1000 K. By comparing the migration energy values of these configurations obtained by nudged elastic band method with those of the Arrhenius fits, we find that the diffusivity for each of single- and di-interstitial atoms in tungsten is a linear function of temperature rather than Arrhenius as usually assumed."> - 必威体育下载

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    Ran Qin, Wang Huan, Zhong Rui, Wu Jian-Chun, Zou Yu, Wang Jun
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    • Abstract views:7462
    • PDF Downloads:103
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    Publishing process
    • Received Date:05 March 2019
    • Accepted Date:08 April 2019
    • Available Online:01 June 2019
    • Published Online:20 June 2019

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