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Anisotropic Friedel oscillations in graphene-like materials: The Dirac point approximation in wave-number dependent quantities revisited

机译:石墨烯类材料中的各向异性弗瑞德振荡:波数相关量的狄拉克点近似

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摘要

Friedel oscillations of the graphene-like materials are investigated theoretically for low and intermediate Fermi energies. Numerical calculations have been performed within the random phase approximation. It was demonstrated that for intra-valley transitions the contribution of the different Dirac points in the wave-number dependent quantities is determined by the orientation of the wave-number in k-space. Therefore, identical contribution of the different Dirac points is not automatically guaranteed by the degeneracy of the Hamiltonian at these points. Meanwhile, it was shown that the contribution of the inter-valley transitions is always anisotropic even when the Dirac points coincide with the Fermi level (EF = 0). This means that the Dirac point approximation based studies could give the correct physics only at long wave length limit. The anisotropy of the static dielectric function reveals different contribution of the each Dirac point. Additionally, the anisotropic k-space dielectric function results in anisotropic Friedel oscillations in graphene-like materials. Increasing the Rashba interaction strength slightly modifies the Friedel oscillations in this family of materials. Anisotropy of the dielectric function in k-space is the clear manifestation of band anisotropy in the graphene-like systems.
机译:理论上研究了低和中等费米能的类石墨烯材料的弗里德振荡。在随机相位近似范围内已进行了数值计算。结果表明,对于谷内跃迁,不同狄拉克点在波数相关量中的贡献取决于波数在k空间中的方向。因此,汉密尔顿算子在这些点上的简并不能自动保证不同狄拉克点的相同贡献。同时,表明即使Dirac点与费米能级(EF = 0)一致,谷间跃迁的贡献也总是各向异性的。这意味着基于狄拉克点近似的研究只能在长波长极限下才能给出正确的物理学。静态介电函数的各向异性揭示了每个狄拉克点的不同贡献。此外,各向异性的k空间介电函数会导致类似石墨烯的材料发生各向异性的Friedel振荡。增加Rashba相互作用强度会稍微改变该系列材料中的Friedel振荡。 k空间中介电函数的各向异性是类石墨烯系统中带各向异性的明显体现。

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