4.4 Article

Plastic deformation of single crystals of Pt3Al with the L12 structure having a far Al-rich off-stoichiometric composition of Pt-29at.%Al

Journal

PHILOSOPHICAL MAGAZINE
Volume 94, Issue 12, Pages 1327-1344

Publisher

TAYLOR & FRANCIS LTD
DOI: 10.1080/14786435.2014.885142

Keywords

platinum aluminide; transmission electron microscopy; intermetallic compound; planar fault energy; dislocation

Funding

  1. JSPS KAKENHI [24246113, 25630304, 25709066]
  2. Elements Strategy Initiative for Structural Materials (ESISM) from the Ministry of Education, Culture, Sports, Science and Technology (MEXT) of Japan
  3. Advanced Low Carbon Technology Research and Development Program (ALCA) from the Japan Science and Technology Agency (JST)
  4. Grants-in-Aid for Scientific Research [25630304, 25709066] Funding Source: KAKEN

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The plastic deformation behaviour of single crystals of Pt3Al with the L1(2) structure having an off-stoichiometric composition of Pt-29at.%Al has been investigated in compression from 77 to 1273 K. The L1(2) phase is stable at least down to 70 K at a composition of Pt-29at.%Al, in contrast to Pt-27at.%Al, in which transformation into a tetragonal phase occurs at around 220 K. Slip occurs along < 1 1 0 > both on (0 0 1) and on (1 1 1) with slip on (0 0 1) being the primary slip system that operates at considerably smaller critical resolved shear stress (CRSS) values in most crystal orientations, except for a narrow orientation region close to [0 0 1]. The CRSSs for both slip on (0 0 1) and (1 1 1) decrease rapidly with increasing temperature at low temperatures, and they are both higher for Pt-29at.%Al than for Pt-27at.%Al due to solid-solution hardening effects. Dislocations with b (Burgers vector) = dissociate into two collinear superpartials with b = 1/2 separated by an APB (anti-phase boundary) on the corresponding slip plane for both slip on (0 0 1) and (1 1 1). The large negative temperature dependence of CRSS for slip on (1 1 1) at low temperatures is not due to the motion of superlattice intrinsic stacking fault (SISF)-coupled superpartials with b = 1/3 < 1 1 2 > but is due to the Peierls mechanism acting on APB-coupled superpartials with a non-planar core structure. The core of APB-coupled superpartials gliding on (0 0 1) is considered to be planar, and hence, the large negative temperature dependence of CRSS for slip on (0 0 1) is due to solid-solution effects arising from the off-stoichiometric composition.

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