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arXiv 1507.05040cond-mat.str-elcond-mat.mtrl-sci
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轨道中的自能和波函数弛豫模型

Modeling the self-energy and wavefunction relaxation in the orbitals

Bolong Huang

摘要:

由于半核3d轨道的边界归一化条件很强,使得这种金属氧化物的线性响应DFT+U在Hubbard U测定中遇到了难以克服的障碍。我们把轨道自能和轨道弛豫作为本征值的分量,各自的轨道占据数遵循费米-狄拉克分布。基于最简单的局域密度形式,采用Hubbard U修正,自洽求解总能量的第二偏偏差,发现在Janak定理成立的情况下,局域密度交换关联势泛函只能给出自能量和轨道弛豫在焦点轨道上的最小余项.这样的残基在完全占据的轨道和非零的部分占据的轨道中被很好地抵消。在保持Janak定域轨道定理有效性的前提下,Hubbard U修正的局域密度泛函自洽循环不能找到一组同时抵消空壳层和部分填充壳层的轨道自能和弛豫的轨道占据,而只能返回一组完全填充壳层的轨道占据.基于自能误差最小化的原则,改进了基于全占据轨道的化合物的带隙计算,并给出了弛豫晶格,为精确研究激发态提供了一条可能的途径.

英文摘要:

The strong boundary normalized condition of wavefunction for fully occupied semicore 3d orbitals leads the linear response DFT+U on such metal oxide to have an insurmountable obstacle in Hubbard U determination. We treated the orbital self-energy and orbital relaxation as components of eigenvalues with respective orbital occupation number that follows the Fermi-Dirac distribution. By self-consistently solving the second partial deviation of total energy based on the most simple local density formalism with Hubbard U correction, we found the local density exchange-correlation potential functional can only give a minimized residue of the self-energy and orbital relaxation on the focus orbital if the Janak theorem maintained. Such residue turns to well counteracted in the fully occupied orbitals and non-zero the partially occupied orbitals. With keeping the validation of Janak theorem on localized orbitals, the self-consistent cycle by local density functional with Hubbard U correction cannot find out a set of orbital occupation that simultaneously offsets the orbital self-energy and relaxations in the empty and partially filled shell, but returns a unique set of the occupation for fully occupied shell. The band gap calculations on fully occupied orbital based compounds are thus improved and the relaxed lattices are also shown based on minimization of the self-energy error, which shows a possible route for accurate excited state studies.

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