Abstract

For improving the thickness and property of WB coating prepared using atomic diffusion theory, the behavior and mechanism for B atom diffusing across W grain boundary (GB) were investigated. The result indicates that, no matter which W GB for B atom diffusing across, stage I (Obulk → S1) decides the diffusion rate, and the energy barrier is not depended on the boundary itself, but controlled by the atomic arrangement structure near GB. W GBs have neighboring octahedral interstices connected by their edges, such as Σ5(210)[001] GB, Σ7(213)[1–20] GB and Σ11(323)[1–31] GB, are the fast diffusion channels for B atom diffusion because of the smaller energy barriers at stage I (≦2.476 eV). While W GBs have neighboring octahedral interstices connected by their faces, including Σ3(111)[1–10] GB, Σ3(112)[1–10] GB, Σ5(210)[001] GB and Σ9(114)[1–10] GB, are the two-dimensional barriers due to the larger energy barriers (>2.476 eV). Both ionic bonding and covalent bonding between B atom at saddle point and the surrounding W atoms at stage I on two-dimensional barriers are stronger than those on fast diffusion channels, which is the reason two-dimensional barriers show the larger energy barriers and the smaller diffusion coefficient for B atom diffusing across.

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