Analysis of magnetic structures of iron nitrides by Landau's theory of second-order phase transitions
Source abstract
Abstract
The magnetic structures of iron nitrides are studied by Landau's theory of second-order phase transitions. It is found that the magnetization direction of ɛ-Fe3N must be parallel to the c-axis of the hexagonal structure, which may conclude the debates on the easy axes of ɛ-Fe3N in this field. The easy axes of α″-Fe16N2 are turned out to be along [001], or [100], or [110] direction, with the former two cases already found by the experiments. The magnetization along [111] is forbidden, which solves rigorously the puzzle why the easy axes of the α″-Fe16N2 on InGaAs and Fe are different from each other. Finally, the magnetic structure of γ′-Fe4N is also determined, and the result shows that there are three possibilities for the magnetization: parallel to the axial, or the body diagonal, or the face diagonal direction of the cubic structure, among which the first case has been found in experiments.
Source: crossref · Quality: baseline
Research context
OpenAlex topics: Magnetic properties of thin films · Magnetic Properties and Applications · Copper Interconnects and Reliability
SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.
Affiliations
Nanjing University 1 Jiangsu Provincial Key Laboratory of Advanced Photonic and Electronic Materials School of Electronics Science and Engineering, Nanjing National Laboratory of Microstructure, , Nanjing 210093, China
Nanjing University of Posts and Telecommunications 2 , Nanjing 210023, China
Department of Physics, Nanjing University 3 , Nanjing 210093, China
References (34)
Show source-provided references
1. Stahl Eisen · 1923 · 12 · 43
2. Appl. Phys. Lett. · 1994 · 64 · 38410.1063/1.111155 ↗
3. J. Alloy. Comp. · 2007 · 443 · 4810.1016/j.jallcom.2007.01.151 ↗
4. J. Alloy. Comp. · 1995 · 227 · 1010.1016/0925-8388(95)01610-4 ↗
5. Nanotechnology · 2005 · 16 · 201210.1088/0957-4484/16/10/005 ↗
6. Phys. Rev. B · 2009 · 80 · 17441210.1103/PhysRevB.80.174412 ↗
7. J. Magn. Magn. Mater. · 1999 · 204 · 19110.1016/S0304-8853(99)00296-6 ↗
8. J. Cryst. Growth · 2007 · 301–302 · 59710.1016/j.jcrysgro.2006.11.041 ↗
9. J. Cryst. Growth · 2007 · 309 · 2510.1016/j.jcrysgro.2007.09.017 ↗
10. J. Alloy. Comp. · 1999 · 288 · 7910.1016/S0925-8388(99)00150-4 ↗
11. J. Phys. Chem. Solids · 1964 · 25 · 71710.1016/0022-3697(64)90182-9 ↗
12. Phys. Status Solids A · 1986 · 98 · 5110.1002/pssa.2210980106 ↗
13. Int. J. Mod. Phys. B · 1993 · 7 · 74110.1142/S0217979293001566 ↗
14. J. Appl. Phys. · 1991 · 70 · 597710.1063/1.350067 ↗
15. Phys. Rev. B · 1971 · 4 · 222410.1103/PhysRevB.4.2224 ↗
16. Phys. Rev. B · 2004 · 70 · 11541710.1103/PhysRevB.70.115417 ↗
17. J. Magn. Magn. Mater. · 2000 · 215–216 · 52910.1016/S0304-8853(00)00210-9 ↗
18. Appl. Phys. Lett. · 2003 · 82 · 328110.1063/1.1573356 ↗
19. Appl. Phys. Lett. · 2003 · 82 · 453410.1063/1.1586790 ↗
20. J. Korean Phys. Soc. · 2012 · 60 · 174510.3938/jkps.60.1745 ↗
21. J. Appl. Phys. · 2011 · 109 · 07E12610.1063/1.3556919 ↗
22. Phys. Rev. B · 2004 · 69 · 14440210.1103/PhysRevB.69.144402 ↗
23. 1958 · 446
24. J. Phys. C: Solid State Phys. · 1975 · 9 · 173110.1088/0022-3719/9/9/015 ↗
25. Phys. Rev. Lett. · 1966 · 17 · 121610.1103/PhysRevLett.17.1216 ↗
26. J. Mater. Chem. · 1999 · 9 · 152710.1039/a809935i ↗
27. 1963 · 67
28. J. Phys. A: Gen. Phys. · 1968 · 1 · 4010.1088/0305-4470/1/1/306 ↗
29. 1972 · 61
30. J. Phys. I France · 1992 · 2 · 181910.1051/jp1:1992248 ↗
31. J. Appl. Phys. · 1996 · 79 · 557610.1063/1.362246 ↗
32. J. Appl. Phys. · 1993 · 73 · 606010.1063/1.353469 ↗
33. J. Appl. Phys. · 1991 · 70 · 603310.1063/1.350084 ↗
34. J. Magn. Magn. Mater. · 2007 · 316 · 32110.1016/j.jmmm.2007.02.187 ↗