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首页> 外文期刊>The American mineralogist >High-pressure behavior of cuprospinel CuFe2O4: Influence of the Jahn-Teller effect on the spinel structure
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High-pressure behavior of cuprospinel CuFe2O4: Influence of the Jahn-Teller effect on the spinel structure

机译:铜氨铜CuFe2O4的高压行为:贾恩-泰勒效应对尖晶石结构的影响

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摘要

The Jahn-Teller effect at Cu2+ in cuprospinel CuFe2O4 was investigated using high-pressure single-crystal synchrotron X-ray diffraction techniques at beamline BL10A at the Photon Factory, KEK, Japan. Six data sets were collected in the pressure range from ambient to 5.9 GPa at room temperature. Structural refinements based on the data were performed at 0.0, 1.8, 2.7, and 4.6 GPa. The unit-cell volume of cuprospinel decreases continuously from 590.8(6) to 579.5(8) angstrom(3) up to 3.8 GPa. Least-squares fitting to a third-order Birch-Murnaghan equation of state yields the zero-pressure volume V-0 = 590.7(1) angstrom(3) and bulk modulus K-0 = 188.1(4.4) GPa with K' fixed at 4.0. The structural formula determined by electron microprobe analysis and site occupancy refinement is represented as (T)(Fe0.903+Cu0.102+)(M)(Fe1.103+Fe0.402+Cu0.502+)O-4. Most of the Cu2+ are preferentially distributed onto the octahedrally coordinated (M) site of the spine! structure. With pressure, the arrangement of the oxygen atoms around the M cation approaches a regular octahedron. This leads to an increase in the electrostatic repulsion between the coordinating oxygen ions and the 3d(z)(2) orbital of Cu-M(2+). At 4.6 GPa, a cubic-tetragonal phase transition is indicated by a splitting of the a axis of the cubic structure into a smaller a axis and a longer c axis, with unit-cell parameters a = 5.882(1) angstrom and c = 8.337(1) angstrom. The tetragonal structure with space group I4(1)/amd was refined to R1= 0.0332 and wR2 = 0.0703 using 38 observed reflections. At the M site, the two M-0 bonds parallel to the c-axis direction of the unit cell are stretched with respect to the four M-O bonds parallel to the a-b plane, which leads to an elongated octahedron along the c-axis. The cubic-to-tetragonal transition induced by the Jahn-Teller effect at Cu2+ is attributable to this distortion of the CuO6 octahedron and involves Cu 3d(z)(2) orbital, ab initio quantum chemical calculations support the observation. At the tetrahedrally coordinated (7) site, on the other hand, the tetrahedral O-T-O bond angle increases from 109.47 degrees to 111.7(7)degrees, which generates a compressed tetrahedral geometry along the c-axis. As a result of the competing distortions between the elongated octahedron and the compressed tetrahedron, the a unit-cell parameter is shortened with respect to the c unit-cell parameter, giving a c/a' ratio (a' = root 2 a) slightly greater than unity as referred to cubic lattice (c/a' = 1.002). The c/a' value increases to 1.007 with pressure, suggesting further distortions of the elongated octahedron and compressed tetrahedron.
机译:在日本KEK光子工厂的光束线BL10A处,使用高压单晶同步加速器X射线衍射技术研究了铜松铜CuFe2O4中Cu2 +的Jahn-Teller效应。在室温下从环境压力到5.9 GPa的压力范围内收集了六个数据集。基于数据的结构优化是在0.0、1.8、2.7和4.6 GPa下进行的。铜硝松的晶胞体积从590.8(6)连续降低到579.5(8)埃(3),最高达到3.8 GPa。最小二乘拟合三阶Birch-Murnaghan状态方程将得出零压力体积V-0 = 590.7(1)埃(3)和体积模量K-0 = 188.1(4.4)GPa,其中K'固定为4.0通过电子探针分析和位置占有率精细化确定的结构式表示为(T)(Fe0.903 + Cu0.102 +)(M)(Fe1.103 + Fe0.402 + Cu0.502 +)O-4。大多数Cu2 +优先分布在脊柱的八面体配位(M)位置!结构体。在压力下,M阳离子周围的氧原子排列接近规则的八面体。这导致配位氧离子与Cu-M(2+)的3d(z)(2)轨道之间的静电排斥力增加。在4.6 GPa时,立方-四边形相变通过将立方结构的a轴分为较小的a轴和较长的c轴来表示,单位像元参数为a = 5.882(1)埃,c = 8.337 (1)埃。使用38个观察到的反射将空间组为I4(1)/ amd的四边形结构精炼为R1 = 0.0332和wR2 = 0.0703。在M位置,平行于晶胞的c轴方向的两个M-0键相对于平行于a-b平面的四个M-O键伸展,这导致沿着c轴的八面体伸长。贾恩-泰勒效应在Cu2 +处诱导的立方到四方转变是由于CuO6八面体的这种畸变引起的,并且涉及Cu 3d(z)(2)轨道,从头算起量子化学计算也支持该观察。另一方面,在四面体配位(7)处,四面体O-T-O键角从109.47度增加到111.7(7)度,沿c轴生成压缩的四面体几何形状。由于细长的八面体和压缩的四面体之间存在竞争性变形,因此相对于c晶胞参数,a晶胞参数会缩短,从而使ac / a'比(a'=根2a)略大比称为立方晶格的单数(c / a'= 1.002)。 c / a'值随着压力增加到1.007,表明细长的八面体和压缩的四面体会进一步变形。

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