Interfacial giant tunnel magnetoresistance and bulk-induced large perpendicular magnetic anisotropy in (111)-oriented junctions with fcc ferromagnetic alloys: A first-principles study
Interfacial giant tunnel magnetoresistance and bulk-induced large perpendicular magnetic anisotropy in (111)-oriented junctions with fcc ferromagnetic alloys: A first-principles study
复制标题
面心立方铁磁合金 (111) 取向结中的界面巨隧道磁阻和体感大垂直磁各向异性:第一性原理研究
DOI:
10.1103/physrevb.103.064427
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发表时间:
2021
影响因子:
3.7
通讯作者:
Miura Yoshio
中科院分区:
文献类型:
--
作者:
Masuda Keisuke;Itoh Hiroyoshi;Sonobe Yoshiaki;Sukegawa Hiroaki;Mitani Seiji;Miura Yoshio
We study the tunnel magnetoresistance (TMR) effect and magnetocrystalline anisotropy in a series of magnetic tunnel junctions (MTJs) with-ordered fcc ferromagnetic alloys and MgO barrier along the [111] direction. Considering the (111)-oriented MTJs with differentalloys, we calculate their TMR ratios and magnetocrystalline anisotropies on the basis of the first-principles calculations. The analysis shows that the MTJs with Co-based alloys (CoNi, CoPt, and CoPd) have high TMR ratios over 2000%. These MTJs have energetically favored Co-O interfaces where interfacial antibonding between Coand Ostates is formed around the Fermi level. We find that the resonant tunneling of the antibonding states, called the interface resonant tunneling, is the origin of the obtained high TMR ratios. Such a mechanism is similar to that found in our recent work on the simple Co/MgO/Co(111) MTJ [K. Masuda , Phys. Rev. B 101, 144404 (2020)2469-995010.1103/PhysRevB.101.144404]. In contrast, different systems have different spin channels where the interface resonant tunneling occurs; for example, the tunneling mainly occurs in the majority-spin channel in the CoNi-based MTJ while it occurs in the minority-spin channel in the CoPt-based MTJ. This means that even though the mechanism is similar, different spin channels contribute dominantly to the high TMR ratio in different systems. Such a difference is attributed to the different exchange splittings in the particular Costates contributing to the tunneling though the antibonding with Ostates. Our calculation of the magnetocrystalline anisotropy shows that manyalloys have large perpendicular magnetic anisotropy (PMA). In particular, CoPt has the largest value of anisotropy energy. We further conduct a perturbation analysis of the PMA with respect to the spin-orbit interaction and reveal that the large PMA in CoPt and CoNi mainly originates from spin-conserving perturbation processes around the Fermi level.