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| 024 | 7 | _ | |a 10.1016/j.jallcom.2014.01.114 |2 doi |
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| 037 | _ | _ | |a FZJ-2014-06421 |
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| 082 | _ | _ | |a 670 |
| 100 | 1 | _ | |a Grushko, Benjamin |0 P:(DE-Juel1)130672 |b 0 |e Corresponding Author |u fzj |
| 245 | _ | _ | |a A refinement of the Al-Ni-Pt phase diagram |
| 260 | _ | _ | |a Lausanne |c 2014 |b Elsevier |
| 336 | 7 | _ | |a Journal Article |b journal |m journal |0 PUB:(DE-HGF)16 |s 1417795681_21915 |2 PUB:(DE-HGF) |
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| 520 | _ | _ | |a Phase equilibria in the Al–Ni–Pt alloy system were specified. The total compositional region of the ternary phase diagram can coarsely be divided into three peculiar subregions. Above ∼70 at.% Al this alloy system is characterized by the formation of complex binary and ternary phases. Between ∼40 and 70 at.% Al the structures based on the CsCl-type configuration dominate, while below ∼40 at.% Al the structures are based on the FCC (Ni, Pt) solid solution. The high-Al subregion was completed with the recently revealed binary high-temperature “Al3Pt” ξ-phase (Bmmb (No. 63), a = 1.9718, b = 1.6228, c = 1.4266 nm), which was found to extend up to 1.6 at.% Ni. In the medium-Al subregion the ternary extension of the Al2Pt phase (β*) separates the compositional regions extending from Al3Ni2 and Al3Pt2. At 900–1100 °C no complete separation was revealed between the compositional fields of the β-phase and β*. With decreasing temperature the total β + β* field shrinks around the compositional lines Al2Pt–Al2NiPt and AlNi–Al2NiPt. In the low-Al subregion the low-Ni limit of the γ♦-phase region, probably extending at low temperatures from Al3Ni5, was found to be below 4 at.%. |
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| 700 | 1 | _ | |a Kapush, Denys |0 P:(DE-Juel1)156590 |b 1 |u fzj |
| 773 | _ | _ | |a 10.1016/j.jallcom.2014.01.114 |0 PERI:(DE-600)2012675-X |p 127 - 132 |t Journal of alloys and compounds |v 594 |y 2014 |x 0925-8388 |
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