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非正交基时变密度泛函理论量子输运模拟。

Time-dependent density functional theory quantum transport simulation in non-orthogonal basis.

机构信息

Department of Chemistry, The University of Hong Kong, Pokfulam Road, Hong Kong.

Hefei National Laboratory for Physical Sciences at the Microscale, University of Science and Technology of China, Hefei, Anhui 230026, China.

出版信息

J Chem Phys. 2013 Dec 14;139(22):224111. doi: 10.1063/1.4840655.

Abstract

Basing on the earlier works on the hierarchical equations of motion for quantum transport, we present in this paper a first principles scheme for time-dependent quantum transport by combining time-dependent density functional theory (TDDFT) and Keldysh's non-equilibrium Green's function formalism. This scheme is beyond the wide band limit approximation and is directly applicable to the case of non-orthogonal basis without the need of basis transformation. The overlap between the basis in the lead and the device region is treated properly by including it in the self-energy and it can be shown that this approach is equivalent to a lead-device orthogonalization. This scheme has been implemented at both TDDFT and density functional tight-binding level. Simulation results are presented to demonstrate our method and comparison with wide band limit approximation is made. Finally, the sparsity of the matrices and computational complexity of this method are analyzed.

摘要

基于量子输运的分层运动方程的早期工作,本文提出了一种通过将含时密度泛函理论(TDDFT)和 Keldysh 非平衡格林函数形式相结合来进行含时量子输运的第一性原理方法。该方法超越了宽带极限近似,并且无需基变换即可直接应用于非正交基的情况。通过将其包含在自能中,适当处理了在引线和器件区域之间的基的重叠,并且可以表明该方法等效于引线-器件的正交化。该方法已在 TDDFT 和密度泛函紧束缚水平上实现。给出了模拟结果以演示我们的方法,并与宽带极限近似进行了比较。最后,分析了该方法的矩阵稀疏性和计算复杂度。

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