journal article·2016-11-22

Room-Temperature Spin Filtering in Metallic Ferromagnet–Multilayer Graphene–Ferromagnet Junctions

Enrique D. Cobas, Olaf M. J. van ’t Erve, Shu-Fan Cheng, James C. Culbertson, Glenn G. Jernigan, Konrad Bussman, Berend T. Jonker

ACS Nano· Volume 10· Issue 11
Publisher page

Abstract

We report room-temperature negative magnetoresistance in ferromagnet-graphene-ferromagnet (FM|Gr|FM) junctions with minority spin polarization exceeding 80%, consistent with predictions of strong minority spin filtering. We fabricated arrays of such junctions via chemical vapor deposition of multilayer graphene on lattice-matched single-crystal NiFe(111) films and standard photolithographic patterning and etching techniques. The junctions exhibit metallic transport behavior, low resistance, and the negative magnetoresistance characteristic of a minority spin filter interface throughout the temperature range 10 to 300 K. We develop a device model to incorporate the predicted spin filtering by explicitly treating a metallic minority spin channel with spin current conversion and a tunnel barrier majority spin channel and extract spin polarization of at least 80% in the graphene layer in our structures. The junctions also show antiferromagnetic coupling, consistent with several recent predictions. The methods and findings are relevant to fast-readout low-power magnetic random access memory technology, spin logic devices, and low-power magnetic field sensors.
Source: openalex_inverted_index · Quality: baseline

Research context

OpenAlex topics: Graphene research and applications · Quantum and electron transport phenomena · Magnetic properties of thin films

SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.

Affiliations

Naval Research Laboratory, 4555 Overlook Avenue SW, Washington D.C. 20375, United States

Funding

U.S. Naval Research Laboratory · Office of Naval Research

References (38)

Show source-provided references
1. 10.1038/nnano.2015.2410.1038/nnano.2015.24 ↗
2. 10.1109/TED.2011.217349810.1109/TED.2011.2173498 ↗
3. 10.1103/PhysRevApplied.5.04400310.1103/PhysRevApplied.5.044003 ↗
4. 10.1021/nl501278c10.1021/nl501278c ↗
5. 10.1038/nature0603710.1038/nature06037 ↗
6. 10.1021/acs.nanolett.6b0049710.1021/acs.nanolett.6b00497 ↗
7. 10.1143/APEX.4.02300310.1143/APEX.4.023003 ↗
8. 10.1103/PhysRevLett.99.17660210.1103/PhysRevLett.99.176602 ↗
9. 10.1103/PhysRevB.80.03540810.1103/PhysRevB.80.035408 ↗
10. 10.1103/PhysRevB.85.18442610.1103/PhysRevB.85.184426 ↗
11. 10.1021/nl300761610.1021/nl3007616 ↗
12. 10.1103/PhysRevB.89.18441810.1103/PhysRevB.89.184418 ↗
13. 10.1038/nnano.2012.16110.1038/nnano.2012.161 ↗
14. 10.1038/ncomms854110.1038/ncomms8541 ↗
15. 10.1038/ncomms416110.1038/ncomms4161 ↗
16. 10.1021/acsnano.5b0279510.1021/acsnano.5b02795 ↗
17. 10.1103/PhysRev.71.62210.1103/PhysRev.71.622 ↗
18. 10.1103/PhysRevB.89.16541710.1103/PhysRevB.89.165417 ↗
19. 10.1007/s12274-013-0314-x10.1007/s12274-013-0314-x ↗
20. 10.1039/c3nr05279f10.1039/c3nr05279f ↗
21. 10.1103/PhysRevB.93.24140110.1103/PhysRevB.93.241401 ↗
22. 10.1021/nn304424x10.1021/nn304424x ↗
23. 10.1063/1.357155310.1063/1.3571553 ↗
24. 10.1063/1.479576410.1063/1.4795764 ↗
25. 10.1103/PhysRevB.58.R291710.1103/PhysRevB.58.R2917 ↗
26. 10.1016/0375-9601(75)90174-710.1016/0375-9601(75)90174-7 ↗
27. 10.1103/PhysRevLett.94.17660110.1103/PhysRevLett.94.176601 ↗
28. 10.1098/rspa.1936.003110.1098/rspa.1936.0031 ↗
29. 10.1103/PhysRevLett.58.227110.1103/PhysRevLett.58.2271 ↗
30. 10.1103/PhysRevB.48.709910.1103/PhysRevB.48.7099 ↗
31. 10.1103/PhysRev.108.117510.1103/PhysRev.108.1175 ↗
32. 10.1016/S0304-8853(99)00316-910.1016/S0304-8853(99)00316-9 ↗
33. 10.1103/PhysRevB.62.R479010.1103/PhysRevB.62.R4790 ↗
34. 10.1103/PhysRevLett.88.02720210.1103/PhysRevLett.88.027202 ↗
35. 10.1088/0953-8984/19/18/18320110.1088/0953-8984/19/18/183201 ↗
36. 10.1016/j.jmmm.2015.10.11310.1016/j.jmmm.2015.10.113 ↗
37. 10.1021/nl061702a10.1021/nl061702a ↗
38. 10.1039/b613962k10.1039/b613962k ↗