The 66th JSAP Spring Meeting, 2019

Presentation information

Oral presentation

10 Spintronics and Magnetics » 10.1 Emerging materials in spintronics and magnetics (including fabrication and charactrization methodologies)

[9p-M101-1~7] 10.1 Emerging materials in spintronics and magnetics (including fabrication and charactrization methodologies)

Sat. Mar 9, 2019 4:00 PM - 6:00 PM M101 (H101)

Hiromi Yuasa(Kyushu univ.)

5:30 PM - 5:45 PM

[9p-M101-6] Electronic and magnetic properties of graphene/Co2Fe(Ge0.5Ga0.5) Heusler alloy heterostructure

〇(P)Songtian Li1, Konstantin V. Larionov2, Zakhar I. Popv2, Yoichi Yamada3, Kenta Amemiya4, Shiro Entani1, Yuya Sakuraba5, Hiroshi Naramto1, Pavel B. Sorokin2, Seiji Sakai1 (1.QST, 2.NUST MISiS, 3.Univ. of Tsukuba, 4.KEK, 5.NIMS)

Keywords:Heusler alloy, Graphene, Spin-valve

As a zero-gap semiconductor with a pin-hole free nature, graphene was proposed as an attractive low energy barrier for vertical spin-valves (SV) to solve the trade-off between MR ratio and low RA product usually observed in MgO-based vertical SV. So far, the MR ratio reported in graphene-spacer vertical SV is far below the application level due to the usage of conventional ferromagnetic electrodes (Ni, Co, Fe etc.) with low spin polarization. Utilizing high spin-polarized ferromagnetic electrodes such as full Heusler alloys is potential way to enhance the MR ratio in graphene-spacer SV, however, there is no precedent for success in the growth of graphene on Heusler alloy underlayer. In this study, we report on the demonstration and characterization of a novel heterostructure consisting of single-layer graphene (SLG) synthesized by high-vacuum chemical vapor deposition (CVD) on a half-metallic Co2Fe(Ge0.5Ga0.5) (CFGG) Heusler alloy, which provides a promising building block for developing high performance graphene-spacer vertical SV.
Fig. 1 shows the surface characterization results of SLG/CFGG/MgO(001) by a, b) RHEED, and c) STM. The sharp RHEED streaks indicate an atomically flap surface of CFGG at the SLG/CFGG interface. The periodic strips in the STM image is attributed to the Moire superstructure resulted from the lattice miss-match between graphene and CFGG(001), indicating the growth of single crystalline SLG on CFGG. Fig. 2 shows the result of the depth-resolved XMCD analysis of the Co L2,3-edge in the SLG/CFGG heterostructure. A robust magnetization was observed in the region just below the SLG/CFGG interface, which indicates little degradation of the magnetic property of the CFGG surface after the CVD-graphene growth. The effect of SLG on the half-metallicity of the CFGG surface will be also discussed in the presentation.