journal article·2015-11-01Open access

The strain induced band gap modulation from narrow gap semiconductor to half-metal on Ti2CrGe: A first principles study

Jia Li, Zhidong Zhang, Zunming Lu, Hongxian Xie, Wei Fang, Shaomin Li, Chunyong Liang, Fuxing Yin

AIP Advances· Volume 5· Issue 11

Abstract

The Heusler alloy Ti2CrGe is a stable L21 phase with antiferromagnetic ordering. With band-gap energy (∼ 0.18 eV) obtained from a first-principles calculation, it belongs to the group of narrow band gap semiconductor. The band-gap energy decreases with increasing lattice compression and disappears until a strain of −5%; moreover, gap contraction only occurs in the spin-down states, leading to half-metallic character at the −5% strain. The Ti1, Ti2, and Cr moments all exhibit linear changes in behavior within strains of −5%– +5%. Nevertheless, the total zero moment is robust for these strains. The imaginary part of the dielectric function for both up and down spin states shows a clear onset energy, indicating a corresponding electronic gap for the two spin channels.
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Research context

OpenAlex topics: Heusler alloys: electronic and magnetic properties · MXene and MAX Phase Materials · 2D Materials and Applications

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Affiliations

Hebei University of Technology 1 School of Science, , Tianjin 300401, People’s Republic of China

Hebei University of Technology 2 Research Institute for Energy Equipment Materials, , Tianjin 300401, People’s Republic of China

Funding

the Youth Research Foundation of Science and Technology for Colleges and Universities of Hebei Province · National Natural Science Foundation of China · Natural Science Foundation of Hebei Province

References (31)

Show source-provided references
1. Phys. Rev. Lett. · 2008 · 100 · 15640410.1103/PhysRevLett.100.156404 ↗
2. Phys. Rev. Lett. · 1983 · 50 · 202410.1103/PhysRevLett.50.2024 ↗
3. von Klitzing · 1996
4. Appl. Phys. Lett. · 2013 · 102 · 02240210.1063/1.4775599 ↗
5. Phys. Rev. B · 2004 · 69 · 14441310.1103/PhysRevB.69.144413 ↗
6. Science · 1998 · 281 · 95110.1126/science.281.5379.951 ↗
7. Phys. Rev. Lett. · 1995 · 74 · 117110.1103/PhysRevLett.74.1171 ↗
8. Phys. Rev. Lett. · 2006 · 97 · 02640110.1103/PhysRevLett.97.026401 ↗
9. Appl. Phys. Lett. · 2013 · 103 · 14240410.1063/1.4823820 ↗
10. J. Phys.: Condens. Matter · 2014 · 26 · 08600310.1088/0953-8984/26/8/086003 ↗
11. Appl. Phys. Lett. · 2011 · 99 · 05250910.1063/1.3619844 ↗
12. J. Magn. Magn. Mater. · 2009 · 321 · L3410.1016/j.jmmm.2009.01.006 ↗
13. J. Phys. D: Appl. Phys. · 2007 · 40 · 150710.1088/0022-3727/40/6/S01 ↗
14. J. Magn. Magn. Matter. · 2008 · 320 · 134510.1016/j.jmmm.2007.11.006 ↗
15. J. of Appl. Phys. · 2009 · 105 · 08371710.1063/1.3116533 ↗
16. Appl. Phys. Lett. · 2009 · 94 · 24250210.1063/1.3156811 ↗
17. Phys. Rev. B · 1996 · 54 · 1116910.1103/PhysRevB.54.11169 ↗
18. Comput. Mater. Sci. · 1996 · 6 · 1510.1016/0927-0256(96)00008-0 ↗
19. Phys. Rev. Lett. · 1996 · 77 · 386510.1103/PhysRevLett.77.3865 ↗
20. Phys. Rev. B · 1992 · 46 · 667110.1103/PhysRevB.46.6671 ↗
21. Phys. Rev. B · 1994 · 50 · 1795310.1103/PhysRevB.50.17953 ↗
22. Phys. Rev. B · 1997 · 55 · 1035510.1103/PhysRevB.55.10355 ↗
23. Phys. Rev. B · 2008 · 78 · 13410610.1103/PhysRevB.78.134106 ↗
24. Phys. Rev. B · 2011 · 84 · 09430210.1103/PhysRevB.84.094302 ↗
25. Phys. Rev. B · 2012 · 86 · 21430110.1103/PhysRevB.86.214301 ↗
26. Phys. Rev. B · 2015 · 91 · 09430610.1103/PhysRevB.91.094306 ↗
27. Phys. Rev. B · 2006 · 73 · 04511210.1103/PhysRevB.73.045112 ↗
28. Acta Phys. Sin. · 2015 · 64 · 07710410.7498/aps.64.077104 ↗
29. 1985
30. Phys. Rev. B · 2007 · 76 · 05411510.1103/PhysRevB.76.054115 ↗
31. Phys. Rev. B · 2005 · 72 · 03520410.1103/PhysRevB.72.035204 ↗