Evaluation of the First Order Ternary Interaction Parameter εBiAsfor Molten Copper

1988 ◽  
Vol 27 (1) ◽  
pp. 23-26 ◽  
Author(s):  
X. H. Jiang ◽  
D. C. Lynch ◽  
W. G. Davenport
2006 ◽  
Vol 71 (3) ◽  
pp. 203-211 ◽  
Author(s):  
Dragana Zivkovic ◽  
Dragan Manasijevic ◽  
Ivan Mihajlovic ◽  
Zivan Zivkovic

The results of calculations of the thermodynamic properties of liquid Ag-In-Sb alloys are presented in this paper. The Redlich-Kister-Muggianu model was used for the calculations. Based on known thermodynamic data for constitutive binary systems and available experimental data for the investigated ternary system, the ternary interaction parameter for the liquid phase in the temperature range 1000-1200 K was determined. Comparison between experimental and calculated results showed their good mutual agreement.


2021 ◽  
Vol 63 (3) ◽  
pp. 315
Author(s):  
А. А. Повзнер ◽  
А.Г. Волков ◽  
Т.А. Ноговицына ◽  
C.А. Бессонов

Concentration and temperature transitions in strongly correlated Fe1-хCoxSi alloys with the Dzyaloshinsky-Moriyya (DM) interaction are considered within the framework of the spin-fluctuation theory and taking into account the results of LDA+U+SO calculations of the density of electronic states. It is shown that order-order concentration transitions with a change in the sign of the left-handed spin chirality (at x <0.2) to right-handed (at 0.2≤x<0.65), and again to left-handed, are associated with a change in the sign of the intermode interaction parameter. At the same time, it was indicated that in the region of compositions Fe1-хCoxSi 0.2≤x<0.65, temperature-prolonged first-order phase transitions appear, accompanied by the appearance of an intermediate temperature region of spin short-range order with uncompensated local magnetization and DM interaction. In an external magnetic field in this temperature range at 0.2<x<0.65, skyrmion microstructures appear. At x=0.65, the intermode interaction parameter becomes zero, and the long-range order becomes ferromagnetic (since the experiment implies compensation for the DM interaction). Instead of a prolonged first-order transition, a second-order temperature transition occurs at х=0.65. The constructed (h-T) diagrams of the magnetic states of Fe1-хCoxSi agree with the experiment.


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