Perpendicular magnetic anisotropy properties of tetragonal Mn3Ga films under various deposition conditions
Source abstract
Abstract
Abstract The tetragonal Mn 3 Ga films exhibited high perpendicular magnetic anisotropy, low saturation magnetization, and high spin polarization, which satisfy the criteria of spin-transfer-torque based devices. For practical device applications, it is necessary to improve the interface nature and optimize the deposition conditions. We fabricated thin films of tetragonal Mn 3 Ga directly on MgO(100) without any buffer layer by using DC/RF magnetron sputtering method. We investigated the crystallinity, microstructure, and magnetic properties with varying the deposition conditions; such as deposition temperature (350–450 °C), RF power (25–40 W), and Ar gas pressure (2–7 mTorr). X-ray diffraction data revealed that the growth direction is perpendicular to the film plane, i.e., the c axis. Scanning electron microscope images showed that the top surface is flat with a maximum thickness of 290 nm. The optimal deposition conditions are 400 °C, 35 W, and 5 mTorr in our sputtering system. For the field perpendicular to the film plane, clear hysteresis loop was observed with the saturation magnetization M S = 100 emu/cc at room temperature. By extrapolating the hard magnetization data for the field parallel to the film plane, the anisotropic energy was estimated about K 1 = 1 × 10 6 J/m 3 .
Source: openaire · Quality: candidate unverified · Source record ↗
Research context
OpenAlex topics: Magnetic properties of thin films · Heusler alloys: electronic and magnetic properties · ZnO doping and properties
SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.
References (17)
Show source-provided references
1. Kurt · Phys. Rev. B · 2011 · 83 · 020405(R)10.1103/PhysRevB.83.020405 ↗
2. Rode · Phys. Rev. B · 2013 · 87 · 18442910.1103/PhysRevB.87.184429 ↗
3. Kharel · J. Phys. Condens. Matter · 2014 · 26 · 12600110.1088/0953-8984/26/12/126001 ↗
4. Kurt · Appl. Phys. Lett. · 2012 · 101 · 23240210.1063/1.4768941 ↗
5. Bai · Appl. Phys. Lett. · 2012 · 100 · 02240810.1063/1.3676195 ↗
6. Yun · J. Phys. Condens. Matter · 2012 · 24 · 41600310.1088/0953-8984/24/41/416003 ↗
7. Feng · J. Korean Phys. Soc. · 2013 · 63 · 105510.3938/jkps.63.1055 ↗
8. Krén · Solid State Commun. · 1970 · 8 · 165310.1016/0038-1098(70)90484-9 ↗
9. Niida · J. Phys. Soc. Jpn. · 1983 · 52 · 151210.1143/JPSJ.52.1512 ↗
10. Niida · J. Appl. Phys. · 1996 · 79 · 594610.1063/1.362115 ↗
11. Balke · Appl. Phys. Lett. · 2007 · 90 · 15250410.1063/1.2722206 ↗
12. Wurmehl · J. Phys. Condens. Matter · 2006 · 18 · 617110.1088/0953-8984/18/27/001 ↗
13. Engel · Phys. Rev. B · 1993 · 48 · 989410.1103/PhysRevB.48.9894 ↗
14. Raquet · Phys. Rev. B · 1996 · 54 · 412810.1103/PhysRevB.54.4128 ↗
15. He · Phys. Rev. B · 2005 · 72 · 15543210.1103/PhysRevB.72.155432 ↗
16. Sucksmith · Proc. Roy. Soc. Lond. A · 1954 · 225 · 36210.1098/rspa.1954.0209 ↗
17. Winterlik · Phys. Rev. B · 2008 · 77 · 05440610.1103/PhysRevB.77.054406 ↗