Browse > Article
http://dx.doi.org/10.4283/JMAG.2015.20.1.001

The First-principles Calculations on the Half-metallic Properties of (001) and (110) Surfaces of Zinc-blende YC  

Bialek, Beata (Department of Physics, Inha University)
Lee, Jae Il (Department of Physics, Inha University)
Publication Information
Abstract
We investigated the half-metallicity and magnetism at the (001) and (110) surfaces of YC in zinc-blende structure by using the all-electron full-potential linearized augmented plane wave method within the generalized gradient approximation. From the calculated local density of states, we found that neither (001) nor (110) surface preserves the half-metallicity. While the magnetic moment of Y atom in the YC bulk is $0.116{\mu}_B$, it is $0.057{\mu}_B$ at the topmost layer of Y-terminated (001) surface. On the contrary, C-terminated (001) YC surface exhibits stronger magnetism than the bulk structure; the calculated magnetic moment on topmost C atom is $1.084{\mu}_B$, while that of C atom in the bulk structure is $0.423{\mu}_B$. The magnetic properties of the non-polar (110) YC surface are slightly enhanced as compared with the bulk structure.
Keywords
half-metal; surface magnetism; first-principles method;
Citations & Related Records
연도 인용수 순위
  • Reference
1 R. A. de Groot, F. M. Mueller, P. G. van Engen, and K. H. J. Bushow, Phys. Rev. Lett. 50, 2024 (1983).   DOI
2 F. Yang, Z. Kang, X. Chen, and Y. Xue, J. Phys. D: Appl. Phys. 46, 325003 (2013).   DOI
3 S. Chadov, T. Graf, K. Chadova, X. Dai, G. H. Fecher, and C. Felser, Phys. Rev. Lett. 107, 047202 (2011).   DOI   ScienceOn
4 I. Galanakis and P. Mavropoulos, Phys. Rev. B 67, 104417 (2003).   DOI   ScienceOn
5 M. S. Miao and W. R. L. Lambrecht, Phys. Rev. B 71, 214405 (2005).   DOI   ScienceOn
6 G. Y. Gao, K. L. Yao, E. Sasioglu, L. M. Sandratskii, Z. L. Liu, and J. L. Jiang, Phys. Rev. B 75, 174442 (2007).   DOI   ScienceOn
7 G. Y. Gao and K. L. Yao, J. Appl. Phys. 106, 053703 (2009).   DOI   ScienceOn
8 G. Y. Gao and K. L. Yao, Appl. Phys. Lett. 91, 082512 (2007).   DOI
9 Q. S. Shao and H. Zhao, J. Supercond. Nov. Magn. 25, 2063 (2012).   DOI
10 G. Y. Gao, K. L. Yao, Z. L. Liu, J. L. Jiang, L. H. Yu, and Y. L. Shi, J. Phys.: Condens. Matt. 19, 315222 (2007).   DOI
11 J. E. Pask, L. H. Yang, C. Y. Fong, W. E. Pickett, and S. Dag, Phys. Rev. B 67, 224420 (2003).   DOI   ScienceOn
12 Y. Xing, Y. Liu, S. N. Li, Y. H. Zhao, and W. H. Xie, Phys. Stat. Sol. B 247, 2268 (2010).   DOI   ScienceOn
13 S. W. Fan, L. J. Ding, Z. L. Wang, and K. L. Yao, Appl. Phys. Lett. 102, 022404 (2013).   DOI   ScienceOn
14 Q. Wu, Z. Wang, S. Fan, and K. Yao, J. Magn. Magn. Mater. 368, 44 (2014).   DOI   ScienceOn
15 W. Kohn and L. J. Sham, Phys. Rev. A 140, 1133 (1965).   DOI
16 E. Wimmer, H. Krakauer, M. Weinert, and A. J. Freeman, Phys. Rev. B 24, 6864 (1981), and references therein.
17 M. Weinert, E. Wimmer, and A. J. Freeman, Phys. Rev. B 26, 4571 (1982).   DOI
18 J. P. Perdew, K. Burke, and M. Ernzerhof, Phys. Rev. Lett. 77, 3865 (1996).   DOI   ScienceOn
19 B. Bialek and J. I. Lee, Solid State Commun. 150, 2138 (2010).   DOI   ScienceOn