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arXiv 1109.4036cond-mat.mtrl-scicond-mat.dis-nn
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随机取代固体的电子结构和自能的密度泛函理论和模型计算

Electronic structure and self energies of randomly substituted solids using density functional theory and model calculations

M. W. Haverkort, I. S. Elfimov, G. A. Sawatzky

摘要:

我们描述的程序,以获得电子结构的无序系统使用紧密结合的模型或相当直接从从头密度泛函能带结构计算。能带结构的计算使用的超级细胞比那些包含一个单一的少数组分原子大得多。我们对大量不同的超级晶胞计算进行平均,这些超级晶胞计算包含超级晶胞中不同随机定位的少数组分原子以及由统计概率加权的不同的少数组分原子总数。我们开发了一个有效的和简单的算法展开这些频带,布洛赫定理的基础上。以这种方式获得的未折叠的能带结构表现出动量和能量加宽的结构,取代了经常使用的单个超级原胞计算中观察到的带隙。使用超级晶胞平均能带结构,可以引入自能,其由随机定位的合金组分的散射产生。自能是因果的,表现出很强的能量和一定的动量依赖性。自能表现出相当不平凡的行为,并且在费米能处通常不为零,导致病态或未定义的费米表面。费米能下的自能实部与明显违反卢廷格定理有关。费米面的表观体积与电子数之间没有简单的关系。介绍了模型和真实的二元合金系统的这些影响的例子。

英文摘要:

We describe procedures to obtain the electronic structure of disordered systems using either tight binding like models or quite directly from ab inito density functional band structure calculations. The band structure is calculated using super cells much larger than those containing a single minority component atom. We average over a large number of different super cell calculations containing different randomly positioned minority component atoms in the super cell as well as a varying total number of minority component atoms, weighted by the statistical probability. We develop an efficient and simple algorithm for unfolding of these bands, based on Bloch's theorem. The unfolded band-structure obtained in this way exhibits momentum and energy broadened structures replacing the gaps observed in often used single super cell calculations. Using the super cell averaged band-structure one can introduce a self-energy, resulting from the scattering of randomly positioned alloy components. The self-energy is causal, and shows strong energy and some momentum dependence. The self-energy shows rather non-trivial behavior and is in general non-zero at the Fermi-energy, resulting in an ill or undefined Fermi surface. The real-part of the self-energy at the Fermi-energy relates to an apparent violation of Luttinger's theorem. There is no simple relation between the apparent Fermi-surface volume and the electron count. Examples introducing these effects both for model and real binary alloy systems are presented.

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