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首页> 外文期刊>Journal of Physics. Condensed Matter >Origin of magnetocrystalline anisotropy oscillations in (001) face-centred-cubic Co thin films and effect of sp-d hybridization
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Origin of magnetocrystalline anisotropy oscillations in (001) face-centred-cubic Co thin films and effect of sp-d hybridization

机译:(001)面心立方Co薄膜中磁晶各向异性振荡的起源和sp-d杂交的影响

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摘要

Magnetocrystalline anisotropy (MA) energy of (001) face-centred-cubic Co(N) films is calculated for film thicknesses N = 1-28 in a realistic tight-binding model with and without sp-d orbital hybridization included. The obtained results show that the average MA energy is not largely influenced by the sp-d hybridization. On the other hand, the oscillation pattern is remarkably changed when the sp-d hybridization is included: in this case the MA energy has oscillations with a clear period of 2 atomic layers (AL), similar to the previous ab initio calculations (Szunyogh L, Ujfalussy B, Blaas C, Pustugova U, Sommers C and Weinberger P 1997 Phys. Rev. B 56 14036). A careful analysis in k- and N-spaces reveals that the total MA oscillations are a superposition of two oscillatory contributions: one coming from the neighbourhood of the (&UGamma;) over bar -point with period close to 2 AL (regardless whether the sp-d hybridization is present or not) and the other originating in the region around the M-point. The (M) over bar -point contribution has a larger period and its amplitude is significantly smaller than that of the (&UGamma;) over bar -point contribution when the sp-d hybridization is included so that the 2 AL (&UGamma;) over bar -point contribution is dominant in this case. The two oscillatory MA contributions are attributed to quantum-well states and the corresponding oscillation periods are related to the extremal radii of the minority-spin bulk Co Fermi surface. [References: 43]
机译:在包括和不包括sp-d轨道杂交的实际紧密结合模型中,针对膜厚度N = 1-28,计算(001)面心立方Co(N)膜的磁晶各向异性(MA)能量。所得结果表明,平均MA能量不受sp-d杂交的很大影响。另一方面,当包括sp-d杂交时,振荡模式会发生显着变化:在这种情况下,MA能量具有清晰的2个原子层(AL)周期的振荡,类似于先前的从头算式(Szunyogh L ,Ujfalussy B,Blaas C,Pustugova U,Sommers C和Weinberger P 1997 Phys。Rev. B 56 14036)。对k和N空间的仔细分析表明,总的MA振荡是两个振荡贡献的叠加:一个来自(-UGamma)邻域在bar点附近,周期接近2 AL(无论sp是否-d杂交的存在与否)和另一个起源于M点附近的区域。当包括sp-d杂交时,(M)超过bar-point的贡献具有较大的周期,并且其幅度显着小于(&UGamma)超过bar-point的贡献,因此2 AL(&UGamma)超过在这种情况下,条点贡献占主导。这两个振荡的MA贡献归因于量子阱态,而相应的振荡周期与少数自旋体块状费米表面的极值半径有关。 [参考:43]

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