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稀土元素镍酸盐中无电荷转移的电荷歧化作为金属-绝缘体转变的一种可能机制。

Charge disproportionation without charge transfer in the rare-earth-element nickelates as a possible mechanism for the metal-insulator transition.

作者信息

Johnston Steve, Mukherjee Anamitra, Elfimov Ilya, Berciu Mona, Sawatzky George A

机构信息

Department of Physics and Astronomy, University of British Columbia, Vancouver, British Columbia, Canada V6T 1Z1 and Quantum Matter Institute, University of British Columbia, Vancouver, British Columbia, Canada V6T 1Z4.

Department of Physics and Astronomy, University of British Columbia, Vancouver, British Columbia, Canada V6T 1Z1.

出版信息

Phys Rev Lett. 2014 Mar 14;112(10):106404. doi: 10.1103/PhysRevLett.112.106404. Epub 2014 Mar 10.

DOI:10.1103/PhysRevLett.112.106404
PMID:24679313
Abstract

We study a model for the metal-insulator (M-I) transition in the rare-earth-element nickelates RNiO3, based upon a negative charge transfer energy and coupling to a rocksaltlike lattice distortion of the NiO6 octahedra. Using exact diagonalization and the Hartree-Fock approximation we demonstrate that electrons couple strongly to these distortions. For small distortions the system is metallic, with a ground state of predominantly d8L character, where L_ denotes a ligand hole. For sufficiently large distortions (δdNi-O∼0.05-0.10  Å), however, a gap opens at the Fermi energy as the system enters a periodically distorted state alternating along the three crystallographic axes, with (d8L_2)S=0(d8)S=1 character, where S is the total spin. Thus the M-I transition may be viewed as being driven by an internal volume "collapse" where the NiO6 octahedra with two ligand holes shrink around their central Ni, while the remaining octahedra expand accordingly, resulting in the (1/2, 1/2, 1/2) superstructure observed in x-ray diffraction in the insulating phase. This insulating state is an example of charge ordering achieved without any actual movement of the charge.

摘要

我们基于负电荷转移能以及与NiO6八面体的岩盐状晶格畸变的耦合,研究了稀土元素镍酸盐RNiO3中金属-绝缘体(M-I)转变的模型。使用精确对角化和哈特里-福克近似,我们证明电子与这些畸变强烈耦合。对于小畸变,系统是金属性的,基态主要具有d8L特征,其中L_表示配体空穴。然而,对于足够大的畸变(δdNi-O∼0.05 - 0.10 Å),当系统进入沿三个晶轴交替的周期性畸变状态时,费米能处会打开一个能隙,具有(d8L_2)S = 0(d8)S = 1特征,其中S是总自旋。因此,M-I转变可被视为由内部体积“坍缩”驱动,其中具有两个配体空穴的NiO6八面体围绕其中心Ni收缩,而其余八面体相应地膨胀,导致在绝缘相中X射线衍射中观察到的(1/2, 1/2, 1/2)超结构。这种绝缘态是在没有任何实际电荷移动的情况下实现电荷有序的一个例子。

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