Abstract
Alloying magnesium (Mg) with rare earth elements such as yttrium (Y) has been reported to activate the pyramidal <c + a> slip systems and improve the plasticity of Mg at room temperature. However, the origins of such dislocations and their dissociation mechanisms remain poorly understood. Here, we systematically investigate these mechanisms using dispersion-inclusive density-functional theory, in combination with molecular dynamics simulations. We find that <c + a> dislocations form more readily on the pyramidal I plane than on the pyramidal II plane in Mg. The addition of Y atoms in Mg facilitates the dissociation of <c + a> dislocations on pyramidal II, leading to the easier formation of the pyramidal II than pyramidal I in Mg-Y alloy. Importantly, in pyramidal II slip plane, a flat potential-energy surface (PES) exists around the position of stable stacking fault energy (SFE), which allows cooperative movement of atoms within the slip plane. Alloying Mg with Y atoms increases the range of the PES, and ultimately promotes different sliding pathways in the Mg-Y alloy. These findings are consistent with experimentally observed activation of the pyramidal II <c + a> slip system in Mg-Y alloys, and provide important insight into the relationship between dislocation structure and macroscopic enhancement of plasticity.
Highlights
Magnesium (Mg) and its alloys are promising candidate materials for energy efficient transportation vehicles and devices due to their high strength and light weight [1,2,3,4]
Following the z-relax method for GSFE calculations, we shift the upper half of the crystal with respect to the lower half of the crystal along the direction
Based on the stacking fault cooperative movement (SFCM) on the stable stacking fault energy (SFE), the pyramidal dislocation can form by following three steps: first, leading partial dislocation slip along 1/3 direction arrives at the position of stable SFE; second, stacking fault migrates cooperatively from off-lattice position to the lattice position; third, trailing partial dislocation starts from the lattice position, just like the inverse process of first process, and does not need to go through the large global unstable SFE (Fig. 3b)
Summary
Magnesium (Mg) and its alloys are promising candidate materials for energy efficient transportation vehicles and devices due to their high strength and light weight [1,2,3,4]. In pyramidal II slip plane, a flat potential-energy surface (PES) exists around the position of stable stacking fault energy (SFE), which allows cooperative movement of atoms within the slip plane. The dislocations on both P1 and P2 plane may dissociate into partials at the position of stable stacking fault energy (SFE) [10,11,12,13].
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