The 83rd JSAP Autumn Meeting 2022

Presentation information

Oral presentation

10 Spintronics and Magnetics » 10.4 Spintronics in semiconductor, topological material, superconductor, and multiferroics

[23a-B201-1~12] 10.4 Spintronics in semiconductor, topological material, superconductor, and multiferroics

Fri. Sep 23, 2022 9:00 AM - 12:15 PM B201 (B201)

Hiroshi Naganuma(Tohoku Univ.), Mitsuharu Uemoto(Kobe Univ.)

12:00 PM - 12:15 PM

[23a-B201-12] Fabrication and characterization of polycrystalline Mn3Sn/Ta structures

〇(D)Takumi Matsuo1, Tomoya Higo1,2,3,4, Hanshen Tsai1,2,3, Daisuke Nishio-Hamane2, Satoru Nakatsuji1,2,3,4,5 (1.Dept. of Phys., Univ. of Tokyo, 2.ISSP, Univ. of Tokyo, 3.JST-CREST, 4.Trans-Quantum Sci. Inst., 5.Johns Hopkins U.)

Keywords:Topological material, Weyl antiferromagnet, Interface

Time-reversal symmetry (TRS) breaking antiferromagnets (AFMs) are recently a topic of interest due to their large responses such as the anomalous Hall effect (AHE) and the anomalous Nernst effect that do not scale with their vanishingly small net magnetization. In the case of the noncollinear Weyl AFM Mn3Sn, these responses can be attributed to the ordering of the cluster magnetic octupole, an order parameter that encapsulates the TRS-breaking spin structure. The magnetic octupole corresponds to the orientation of a pair of Weyl points in momentum space. In thin films of Mn3Sn, the octupole can be switched by a spin current injected from a neighboring layer with strong spin-orbit coupling, most commonly a heavy metal (HM). To study surface-dependent effects in Mn3Sn such as spin-orbit torque, thinner films and smoother interfaces with other materials are desired.
Our work focuses on polycrystalline Mn3Sn/Ta bilayers, where Ta caps the Mn3Sn layer due to the prospect of using it as a spin source. We show that the immiscibility of these two materials allows for greater flexibility in the fabrication process than when HM = Pt, W. Transmission electron microscopy and atomic force microscope reveal that the resultant films yield a smoother Mn3Sn/HM interface (RMS ~ 0.5 nm) compared to conventionally prepared polycrystalline films. Furthermore, where previous works report Mn3Sn films with thicknesses above 30 nm, large anomalous Hall conductivity comparable to that of bulk crystals was retained in our Mn3Sn layers as thin as 20 nm.