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SrFeIrO: 扩展氧化物中的平面正方形 Ir(II)。

SrFeIrO: Square-Planar Ir(II) in an Extended Oxide.

机构信息

Department of Chemistry , University of Oxford, Inorganic Chemistry Laboratory , South Parks Road , Oxford OX1 3QR , U.K.

ISIS Facility, Rutherford Appleton Laboratory , Chilton, Oxon OX11 0QX , U.K.

出版信息

Inorg Chem. 2018 Nov 5;57(21):13577-13585. doi: 10.1021/acs.inorgchem.8b02198. Epub 2018 Oct 9.

DOI:10.1021/acs.inorgchem.8b02198
PMID:30299947
Abstract

Topochemical reduction of the double-perovskite oxide SrFeIrO under dilute hydrogen leads to the formation of SrFeIrO. This phase consists of ordered infinite sheets of apex-linked FeO and IrO squares stacked with Sr cations and is the first report of Ir in an extended oxide phase. Plane-wave density functional theory calculations indicate high-spin Fe (d, S = 2) and low-spin Ir (d, S = /) configurations for the metals and confirm that both ions have a doubly occupied d orbital, a configuration that is emerging as a consistent feature of all layered oxide phases of this type. The stability and double occupation of d in the Ir ions invites a somewhat unexpected analogy to the extensively studied Ir ion as both ions share a common near-degenerate (d ) valence configuration. On cooling below 115 K, SrFeIrO enters a magnetically ordered state in which the Ir and Fe sublattices adopt type II antiferromagnetically coupled networks which interpenetrate each other, leading to frustration in the nearest-neighbor Fe-O-Ir couplings, half of which are ferromagnetic and half antiferromagnetic. The spin frustration drives a symmetry-lowering structural distortion in which the four equivalent Ir-O and Fe-O distances of the tetragonal I4/ mmm lattice split into two mutually trans pairs in a lattice with monoclinic I112/ m symmetry. This strong magneto-lattice coupling arises from the novel local electronic configurations of the Fe and Ir cations and their cation-ordered arrangement in a distorted perovskite lattice.

摘要

在稀释的氢气中,对双钙钛矿氧化物 SrFeIrO 进行拓扑化学还原会生成 SrFeIrO。该相由顶点相连的 FeO 和 IrO 正方形无限层组成,层间堆叠 Sr 阳离子,这是 Ir 出现在扩展氧化物相中的首例报道。平面波密度泛函理论计算表明金属中 Fe(d,S=2)和 Ir(d,S=1/2)具有高自旋和低自旋构型,并证实两种离子都具有占据的 d 轨道,这种构型正在成为此类所有层状氧化物相的一致特征。Ir 离子的 d 轨道的稳定性和双重占据使得其与广泛研究的 Ir 离子具有某种出人意料的类比性,因为两种离子都具有共同的近简并(d)价态构型。在冷却至 115 K 以下时,SrFeIrO 进入磁有序状态,其中 Ir 和 Fe 亚晶格采用 II 型反铁磁耦合网络,相互贯穿,导致相邻 Fe-O-Ir 键合的受挫,其中一半为铁磁,一半为反铁磁。自旋受挫导致对称性降低的结构畸变,其中四方 I4/mmm 晶格的四个等效 Ir-O 和 Fe-O 距离分裂成具有单斜 I112/ m 对称性的晶格中的两对相互平移对。这种强烈的磁-晶格耦合源于 Fe 和 Ir 阳离子的新型局部电子构型及其在扭曲钙钛矿晶格中的有序排列。

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