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首页> 外文期刊>Physical Review, B. Condensed Matter >Ferromagnetic zigzag chains and properties of the charge-ordered perovskite manganites - art. no. 174406
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Ferromagnetic zigzag chains and properties of the charge-ordered perovskite manganites - art. no. 174406

机译:铁磁之字形链和带电有序钙钛矿锰矿的特性-艺术。没有。 174406

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摘要

The low-temperature properties of the so-called ''charge-ordered'' state in 50% doped perovskite manganites are described from the viewpoint of the magnetic spin ordering. In these systems, the zigzag antiferromagnetic ordering, combined with the double exchange physics, effectively divides the whole sample into the one-dimensional ferromagnetic zigzag chains and results in the anisotropy of electronic properties. The electronic structure of one such chain is described by an effective 3x3 Hamiltonian in the basis of Mn(3de(g)) orbitals. We treat this problem analytically and consider the following properties: (i) the nearest-neighbor magnetic interactions; (ii) the distribution of the Mn(3 de(g)) and Mn(4p) states near the Fermi level, and their contribution to the optical conductivity and the resonant x-ray scattering near the Mn K-absorption edge. We argue that the anisotropy of magnetic interactions in the double exchange limit, combined with the isotropic superexchange interactions, readily explains both the local and the global stability of the zigzag antiferromagnetic state. The twofold degeneracy of e(g) levels plays a very important role in the problem and explains the insulating behavior of the zigzag chain, as well as the appearance of the orbital ordering in the double exchange model. Importantly, however, the charge ordering itself is expected to play only a minor role and is incompatible with the ferromagnetic coupling within the chain. We also discuss possible effects of the Jahn-Teller distortion and compare the tight-binding picture with results of band-structure calculations in the local-spin-density approximation. [References: 50]
机译:从磁自旋有序的角度描述了50%掺杂钙钛矿锰矿中所谓的``电荷有序''状态的低温特性。在这些系统中,之字形反铁磁有序与双重交换物理学相结合,有效地将整个样本划分为一维铁磁之字形链,并导致电子特性的各向异性。一个这样的链的电子结构在Mn(3de(g))轨道的基础上由有效的3x3哈密顿量来描述。我们通过分析来处理该问题,并考虑以下特性:(i)最近邻的磁相互作用; (ii)费米能级附近的Mn(3 de(g))和Mn(4p)态的分布,以及它们对光导率和Mn K吸收边缘附近的共振X射线散射的贡献。我们认为,在双交换极限中的磁相互作用的各向异性,以及各向同性的超交换相互作用,很容易解释了之字形反铁磁态的局部和全局稳定性。 e(g)能级的双重简并性在该问题中起着非常重要的作用,并解释了之字形链的绝缘行为以及双交换模型中轨道有序的出现。但是,重要的是,电荷排序本身仅会扮演很小的角色,并且与链中的铁磁耦合不兼容。我们还讨论了Jahn-Teller失真的可能影响,并在局部自旋密度近似中将紧束缚图片与能带结构计算的结果进行比较。 [参考:50]

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