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YBaFe₂O₅中的混合价态

Mixed valence in YBaFe(2)O(5).

作者信息

Woodward Patrick M, Karen Pavel

机构信息

Department of Chemistry, The Ohio State University, 100 West 18th Avenue, Columbus, Ohio 43210-1185, USA.

出版信息

Inorg Chem. 2003 Feb 24;42(4):1121-9. doi: 10.1021/ic026022z.

Abstract

YBaFe(2)O(5) has been synthesized by heating a nanoscale citrate precursor in a carefully controlled reducing environment. Successful synthesis of a single-phase sample can only be achieved in a narrow window of oxygen partial pressures and temperatures. YBaFe(2)O(5) adopts an oxygen-deficient perovskite-type structure, which contains double layers of corner sharing FeO(5) square pyramids separated by Y(3+) ions. At T(N) congruent with 430 K, tetragonal (P4/mmm) and paramagnetic YBaFe(2)O(5) orders antiferromagnetically (AFM) experiencing a slight orthorhombic distortion (Pmmm). Around this temperature, it can be characterized as a class-III mixed valence (MV) compound, where all iron atoms exist as equivalent MV Fe(2.5+) ions. The magnetic structure is characterized by AFM Fe-O-Fe superexchange coupling within the double layers and a ferromagnetic Fe-Fe direct-exchange coupling between neighboring double layers. Upon cooling below approximately 335 K, a premonitory charge ordering (2Fe(2.5+) --> Fe(2.5+delta) + Fe(2.5)(-delta)) into a class-II MV phase takes place. This transition is detected by differential scanning calorimetry, but powder diffraction techniques fail to detect any volume change or a long-range structural order. At approximately 308 K, a complete charge ordering (2Fe(2.5+) --> Fe(2+) + Fe(3+)) into a class-I MV compound takes place. This charge localization triggers a number of changes in the crystal, magnetic, and electronic structure of YBaFe(2)O(5). The magnetic structure rearranges to a G-type AFM structure, where both the Fe-O-Fe superexchange and the Fe-Fe direct-exchange couplings are antiferromagnetic. The crystal structure rearranges (Pmma) to accommodate alternating chains of Fe(2+) and Fe(3+) running along b and an unexpectedly large cooperative Jahn-Teller distortion about the high-spin Fe(2+) ions. This order of charges does not fulfill the Anderson condition, and it rather corresponds to an ordering of doubly occupied Fe(2+) d(xz) orbitals. Comparisons with YBaMn(2)O(5) and YBaCo(2)O(5) are made to highlight the impact of changing the d-electron count.

摘要

通过在精心控制的还原环境中加热纳米级柠檬酸盐前驱体合成了YBaFe₂O₅。只有在氧气分压和温度的狭窄窗口内才能成功合成单相样品。YBaFe₂O₅采用缺氧钙钛矿型结构,其中包含由Y³⁺离子隔开的角共享FeO₅四方金字塔双层。在Tₙ≈430K时,四方(P4/mmm)和顺磁性的YBaFe₂O₅发生反铁磁(AFM)有序化,同时经历轻微的正交畸变(Pmmm)。在这个温度附近,它可以被表征为III类混合价(MV)化合物,其中所有铁原子都以等效的MV Fe².⁵⁺离子形式存在。磁结构的特征是双层内的AFM Fe-O-Fe超交换耦合以及相邻双层之间的铁磁Fe-Fe直接交换耦合。在冷却至约335K以下时,会发生预电荷有序化(2Fe².⁵⁺→Fe².⁵⁺⁺δ+Fe².⁵⁻⁺δ)进入II类MV相。这种转变通过差示扫描量热法检测到,但粉末衍射技术未能检测到任何体积变化或长程结构有序化。在约308K时,会发生完全电荷有序化(2Fe².⁵⁺→Fe²⁺+Fe³⁺)进入I类MV化合物。这种电荷局域化引发了YBaFe₂O₅晶体、磁性和电子结构的许多变化。磁结构重新排列为G型AFM结构,其中Fe-O-Fe超交换和Fe-Fe直接交换耦合都是反铁磁的。晶体结构重新排列(Pmma)以适应沿b方向交替排列的Fe²⁺和Fe³⁺链以及围绕高自旋Fe²⁺离子的意外大的协同 Jahn-Teller 畸变。这种电荷有序化不满足安德森条件,而是对应于双占据Fe²⁺ d(xz)轨道的有序化。与YBaMn₂O₅和YBaCo₂O₅进行了比较,以突出改变d电子数的影响。

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