2017
DOI: 10.1016/j.actamat.2016.10.042
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Comprehensive first-principles study of stable stacking faults in hcp metals

Abstract: The plastic deformation in hcp metals is complex, with the associated dislocation core structures and properties not well understood on many slip planes in most hcp metals. A first step in establishing the dislocation properties is to examine the stable stacking fault energy and its structure on relevant slip planes. However, this has been perplexing in the hcp structure due to additional in-plane displacements on both side of the slip plane. Here, density functional theory guided by crystal symmetry analysis … Show more

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Cited by 163 publications
(73 citation statements)
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“…The largest Peierls stress observed was 365 MPa for the dislocation on the {101} plane at 0K, which is in par with the experimental observation, see [32]. properties, as shown in a recent study for hcp metals [42]. Nevertheless, in this work for the first time a systematic study was carried out to assess the dislocation properties along the various non-equivalent slip system in β-Sn.…”
Section: Discussionsupporting
confidence: 79%
“…The largest Peierls stress observed was 365 MPa for the dislocation on the {101} plane at 0K, which is in par with the experimental observation, see [32]. properties, as shown in a recent study for hcp metals [42]. Nevertheless, in this work for the first time a systematic study was carried out to assess the dislocation properties along the various non-equivalent slip system in β-Sn.…”
Section: Discussionsupporting
confidence: 79%
“…In general, we find that there is agreement between the GPT and aGPT at the stable stacking fault. However, for the unstable stacking fault the aGPT improves upon the GPT relative to the DFT results of Yin et al 31…”
Section: B Stacking Fault Energiesmentioning
confidence: 62%
“…whereG αβ (ε) = γh γαhγβ is the strained metric tensor. If the strain is sufficiently small so as to vanish at quadratic order ε αβ = δε αβ , we may write G αβ (ε) = G αβ + 2 µν δε µν h µα h νβ (31) where G αβ is the metric tensor of the unstrained crystal. By denoting the second term as δG αβ and expanding Eq.29 about δG = 0, we find…”
Section: B Stress Tensormentioning
confidence: 99%
“…In this paper we use first principles methods to compute the entire γ-surface for a generalised fault lying between {0111} atomic planes with the larger spacing. Faults between widely spaced {0111} atomic planes are relevant to c + a slip, while faults between narrowly spaced {0111} atomic planes are relevant to a slip [13].…”
Section: Introductionmentioning
confidence: 99%
“…We will show that there is no stable stacking fault in α-Ti with a fault vector of ≈ 1 2 (c + a). Yin et al [13] used symmetry arguments and a hard sphere model to identify approximate translation vectors of possible stable stacking faults without calculating the full γ surfaces. They then carried out full relaxations of these faults using DFT for six hcp metals including Ti.…”
Section: Introductionmentioning
confidence: 99%