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Magnetic decoupling of Fe coverage across atomic step of MoS2 flakes on SiO2 surface.

Authors :
Chuan-Che Hsu
Zong-You Lin
Po-Chun Chang
Hsiang-Chih Chiu
Hsiao-Wen Chen
Hsiang-Lin Liu
Francesco Bisio
Wen-Chin Lin
Source :
Journal of Physics D: Applied Physics; 10/18/2017, Vol. 50 Issue 41, p1-1, 1p
Publication Year :
2017

Abstract

In this study, we deposited Fe films on MoS<subscript>2</subscript> flakes, and investigated the microscopic magnetic behavior on individual flakes. The MoS<subscript>2</subscript> flakes were fabricated on SiO<subscript>2</subscript>/Si(1 0 0) substrates using chemical vapor deposition. Fe coverage was deposited on the MoS<subscript>2</subscript> flakes by e-beam evaporation with a thin Pd capping for protection. Investigations by atomic force microscope and Raman spectroscopy confirmed that the MoS<subscript>2</subscript> flakes had a mean lateral size of 10–20 μ m and mostly single layer thick. After depositing 3.6 and 7.0 nm Fe on MoS<subscript>2</subscript>/SiO<subscript>2</subscript>, clear hysteresis loops were observable with the in-plane magnetic field. From the investigation using a magneto-optical Kerr microscope, we measured the hysteresis curves within individual MoS<subscript>2</subscript> flakes. Although the Fe coverage was much thicker than the MoS<subscript>2</subscript> atomic step height (∼0.66 nm) and the direct connection and strong ferromagnetic coupling between Fe/MoS<subscript>2</subscript> and Fe/SiO<subscript>2</subscript> were expected, a magnetic decoupling between the magnetic domains of Fe/MoS<subscript>2</subscript> and Fe/SiO<subscript>2</subscript> was surprisingly observed. For 3.6 nm Fe/MoS<subscript>2</subscript>, the magnetic coercivity (H<subscript>c</subscript>) was 28  ±  5 Oe, while in contrast, the H<subscript>c</subscript> of 3.6 nm Fe/SiO<subscript>2</subscript> ranged 58  ±  5 Oe. With a thicker Fe coverage of 7.0 nm, the H<subscript>c</subscript> of Fe/MoS<subscript>2</subscript> and Fe/SiO<subscript>2</subscript> converged and the magnetic decoupling became too weak to observe. The distinct interface magnetic anisotropy of Fe on different substrates was held responsible for the observed magnetic decoupling across the MoS<subscript>2</subscript> atomic step between Fe/MoS<subscript>2</subscript> and Fe/SiO<subscript>2</subscript> domains. These observations will be valuable in combining a magnetic coverage with a single layer MoS<subscript>2</subscript> for future spintronic applications. [ABSTRACT FROM AUTHOR]

Details

Language :
English
ISSN :
00223727
Volume :
50
Issue :
41
Database :
Complementary Index
Journal :
Journal of Physics D: Applied Physics
Publication Type :
Academic Journal
Accession number :
125368797
Full Text :
https://doi.org/10.1088/1361-6463/aa86d2