Temperature dependence of the stacking-fault Gibbs energy for Al, Cu, and Ni

被引:67
|
作者
Zhang, Xi [1 ]
Grabowski, Blazej [1 ]
Koermann, Fritz [1 ,2 ]
Ruban, Andrei V. [3 ,4 ]
Gong, Yilun [5 ]
Reed, Roger C. [1 ,5 ,6 ]
Hickel, Tilmann [1 ]
Neugebauer, Joerg [1 ]
机构
[1] Max Planck Inst Eisenforsch GmbH, Dept Computat Mat Design, Max Planck Str 1, D-40237 Dusseldorf, Germany
[2] Delft Univ Technol, Dept Mat Sci & Engn, Mekelweg 2, NL-2628 CD Delft, Netherlands
[3] KTH Royal Inst Technol, Dept Mat Sci & Engn, SE-10044 Stockholm, Sweden
[4] Mat Ctr Leoben, A-8700 Leoben, Austria
[5] Univ Oxford, Dept Mat, Parks Rd, Oxford OX1 3PH, England
[6] Univ Oxford, Dept Engn Sci, Parks Rd, Oxford OX1 3PJ, England
基金
欧洲研究理事会;
关键词
DENSITY-FUNCTIONAL THEORY; COHERENT TWIN BOUNDARIES; AB-INITIO CALCULATION; PLASTIC-DEFORMATION; DISLOCATION LOOPS; 1ST-PRINCIPLES CALCULATIONS; INTERFACIAL ENERGY; SINGLE-CRYSTALS; CLIMB KINETICS; POINT-DEFECTS;
D O I
10.1103/PhysRevB.98.224106
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
The temperature-dependent intrinsic stacking fault Gibbs energy is computed based on highly converged density-functional-theory (DFT) calculations for the three prototype face-centered cubic metals Al, Cu, and Ni. All relevant temperature-dependent contributions are considered including electronic, vibrational, magnetic, and explicit anharmonic Gibbs energy contributions as well as coupling terms employing state-of-the-art statistical sampling techniques. Particular emphasis is put on a careful comparison of different theoretical concepts to derive the stacking fault energy such as the axial-next-nearest-neighbor-Ising (ANNNI) model or the vacuum-slab approach. Our theoretical results are compared with an extensive set of previous theoretical and experimental data. Large uncertainties in the experimental data highlight the necessity of complementary parameter-free calculations. Specifically, the temperature dependence is experimentally unknown and poorly described by thermodynamic databases. Whereas CALPHAD derived data shows an increase of the stacking fault energy with temperature for two of the systems (Cu and Ni), our results predict a decrease for all studied systems. For Ni, the temperature induced change is in fact so strong that in the temperature interval relevant for super-alloy applications the stacking fault energy falls below one third of the low temperature value. Such large changes clearly call for a revision of the stacking fault energy when modeling or designing alloys based on such elements.
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页数:24
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