Spin-polarized currents generated by magnetic Fe atomic chains
Source abstract
Abstract
Fe-based devices are widely used in spintronics because of high spin-polarization and magnetism. In this work, freestanding Fe atomic chains, the thinnest wires, were used to generate spin-polarized currents due to the spin-polarized energy bands. By ab initio calculations, the zigzag structure was found to be more stable than the wide-angle zigzag structure and had a higher ratio of spin-up and spin-down currents. By our theoretical prediction, Fe atomic chains have a sufficiently long thermal lifetime only at T ≦̸ 150 K, while C atomic chains are very stable even at T = 1000 K. This means that the spintronic devices based on Fe chains could work only at low temperatures. A system constructed by a short Fe chain sandwiched between two graphene electrodes could be used as a spin-polarized current generator, while a C chain could not be used in this way. The present work may be instructive and meaningful to further practical applications based on recent technical developments on the preparation of metal atomic chains (Proc. Natl. Acad. Sci. USA 107 9055 (2010)).
Source: openalex_inverted_index · Quality: baseline
Research context
OpenAlex topics: Molecular Junctions and Nanostructures · Quantum and electron transport phenomena · Graphene research and applications
SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.
References (46)
Show source-provided references
1. 10.1126/science.106538910.1126/science.1065389 ↗
2. 10.1103/RevModPhys.76.32310.1103/RevModPhys.76.323 ↗
3. 10.1103/RevModPhys.80.151710.1103/RevModPhys.80.1517 ↗
4. 10.1038/nature0518010.1038/nature05180 ↗
5. 10.1063/1.353796510.1063/1.3537965 ↗
6. 10.1103/PhysRevB.80.07340110.1103/PhysRevB.80.073401 ↗
7. 10.1103/PhysRevLett.101.11550210.1103/PhysRevLett.101.115502 ↗
8. 10.1038/2739910.1038/27399 ↗
9. 10.1038/2740510.1038/27405 ↗
10. 10.1103/PhysRevLett.81.444810.1103/PhysRevLett.81.4448 ↗
11. 10.1103/PhysRevLett.85.412410.1103/PhysRevLett.85.4124 ↗
12. 10.1103/PhysRevB.48.1472110.1103/PhysRevB.48.14721 ↗
13. 10.1103/PhysRevB.80.20540610.1103/PhysRevB.80.205406 ↗
14. 10.1103/PhysRevLett.102.20550110.1103/PhysRevLett.102.205501 ↗
15. Mikhailovskij I M · Nanotech. · 2007 · 1810.1088/0957-4484/18/47/475705 ↗
16. 10.1021/nl803399j10.1021/nl803399j ↗
17. 10.1103/PhysRevB.80.16540410.1103/PhysRevB.80.165404 ↗
18. 10.1103/physrevb.81.08543910.1103/physrevb.81.085439 ↗
19. 10.1021/ja044526l10.1021/ja044526l ↗
20. 10.1002/anie.v48:4210.1002/anie.v48:42 ↗
21. 10.1038/nchem.82810.1038/nchem.828 ↗
22. 10.1021/nl080067110.1021/nl0800671 ↗
23. 10.1103/PhysRevB.87.16140610.1103/PhysRevB.87.161406 ↗
24. 10.1073/pnas.091497010710.1073/pnas.0914970107 ↗
25. 10.1103/PhysRevB.75.20541910.1103/PhysRevB.75.205419 ↗
26. 10.1103/PhysRevB.85.16541210.1103/PhysRevB.85.165412 ↗
27. 10.1103/PhysRevB.87.08510810.1103/PhysRevB.87.085108 ↗
28. 10.1103/PhysRevB.72.18440710.1103/PhysRevB.72.184407 ↗
29. 10.1063/1.345799810.1063/1.3457998 ↗
30. 10.1063/1.477309910.1063/1.4773099 ↗
31. Lin Z-Z · EPL · 2011 · 95
32. Lin Z-Z · EPL · 2013 · 101
33. 10.1103/PhysRevA.87.04340510.1103/PhysRevA.87.043405 ↗
34. Yu W-F · Chin. Phys. · 2013 · 22
35. Soler J M · J. Phys.: Condens. Matter · 2002 · 14 · 274510.1088/0953-8984/14/11/302 ↗
36. 10.1103/PhysRevLett.77.386510.1103/PhysRevLett.77.3865 ↗
37. 10.1103/PhysRevB.43.199310.1103/PhysRevB.43.1993 ↗
38. 10.1103/PhysRevB.65.16540110.1103/PhysRevB.65.165401 ↗
39. 10.1103/PhysRevB.31.620710.1103/PhysRevB.31.6207 ↗
40. 10.1103/PhysRevB.77.21441310.1103/PhysRevB.77.214413 ↗
41. 10.1103/PhysRevB.70.04541710.1103/PhysRevB.70.045417 ↗
42. 10.1103/PhysRevB.77.15543710.1103/PhysRevB.77.155437 ↗
43. 10.1103/PhysRevB.69.02440410.1103/PhysRevB.69.024404 ↗
44. 10.1103/PhysRevB.76.13220110.1103/PhysRevB.76.132201 ↗
45. 10.1103/PhysRevB.80.11542010.1103/PhysRevB.80.115420 ↗
46. 10.1021/ja106925f10.1021/ja106925f ↗