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arXiv 0804.3768cond-mat.supr-concond-mat.mtrl-sci
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Na $_x$ CoO $_2$中a $_{1g}$和e $_g$ '排序的起源

The origin of a$_{1g}$ and e$_g$' orderings in Na$_x$CoO$_2$

D. Pillay, M. D. Johannes, I. I. Mazin, O. K. Andersen

摘要:

在NaxCoO_2中,由于相关效应的存在,导致了LDA所预言的小e_g'费米面口袋的出现,而ARPES测量中没有发现这种现象。在动力学平均场论(DMFT)中,只有在考虑局域关联效应之前,eg'络合物的在位能量低于a1 g络合物的在位能量,才能再现ARPES。目前关于两个轨道复合物的数量级的估计范围从-200 meV到315 meV,以能量差为单位。在这项工作中,我们进行了密度泛函理论计算的单电子分裂Δ= ε_a1g-ε_e_g'的完整的两层化合物,Na_2xCo_2 O_4,占Na有序,面间相互作用和八面体畸变的影响。我们发现对于所有的Na填充物,εa_1g-εe_g'都是负的,这主要是由于Na+离子在插入层中产生的强正库仑场所致。这个场不成比例地影响a_1g轨道,a_1g轨道比e_g'轨道从Co平面向上突出得更远。我们还讨论了八面体压缩和多轨道填充对Δ值随Na含量变化的次级效应。我们的结果表明,如果e_g'口袋确实被抑制,这只能是由于非局部相关效应超出了标准DMFT。

英文摘要:

It has often been suggested that correlation effects suppress the small e_g' Fermi surface pockets of NaxCoO_2 that are predicted by LDA, but absent in ARPES measurements. It appears that within the dynamical mean field theory (DMFT) the ARPES can be reproduced only if the on-site energy of the eg' complex is lower than that of the a1g complex at the one-electron level, prior to the addition of local correlation effects. Current estimates regarding the order of the two orbital complexes range from -200 meV to 315 meV in therms of the energy difference. In this work, we perform density functional theory calculations of this one-electron splitting Δ= ε_a1g-ε_e_g' for the full two-layer compound, Na2xCo2O4, accounting for the effects of Na ordering, interplanar interactions and octahedral distortion. We find that εa_1g-εe_g' is negative for all Na fillings and that this is primarily due to the strongly positive Coulomb field created by Na+ ions in the intercalant plane. This field disproportionately affects the a_1g orbital which protrudes farther upward from the Co plane than the e_g' orbitals. We discuss also the secondary effects of octahedral compression and multi-orbital filling on the value of Δas a function of Na content. Our results indicate that if the e_g' pockets are indeed suppressed that can only be due to nonlocal correlation effects beyond the standard DMFT.

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