铈氢化物的有序-无序转变,在温度依赖的拉曼散射光谱中表现出来

IF 3.2 3区 化学 Q2 CHEMISTRY, PHYSICAL
Shahar Aziza, Soshi Iimura, Chengyu Jin, Karin Fink, Shmuel Hayun* and Tsachi Livneh*, 
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引用次数: 0

摘要

在77 ~ 345 K范围内,研究了CeH2+x (x = 0.25、0.50、0.79和0.94)的声子和电子拉曼散射。dft计算的声子色散曲线和Ce3+晶体场态能量的嵌入团簇模型从头计算在理论上支持了实验分析,并与广泛研究的镧系氢化物“孪生体系”相关,该体系表现出高度相似的温度-组成相图。CeH2.94的拉曼光谱主要由一个频率位于计算得到的bif3型立方CeH3声子色散曲线的能隙内的频带所支配。这一结果与结构修饰有关,由H从预期的Wyckoff位置位移驱动,特别是与额外的正交相一起,理论上证明了LaH ~ 3是两相中动态稳定的相。八面体h -亚晶格重排受到H-H相互作用的强烈影响,可以驱动镧系氢化物中随温度变化的有序-无序转变。0.7 < x <; 0.8的氢化物在~ 245 K时经历了电子(金属-半导体)转变,伴随着结构(立方-四方)相变。在这里,我们通过监测四面体h -亚晶格声子,以及跟踪Ce3+离子周围晶体场方案的变化,系统地证明了拉曼散射密切关注CeH2.79的这种转变的能力。在CeH2.25和CeH2.50镧“孪晶体系”中,在~ 200 K以下形成的长程四方有序结构表现在其衍射图的温度演化上。然而,尽管具有明确结构的固体的一阶拉曼散射光谱是由布里渊Γ-point对称性允许的声子组成的,但CeH2.25拉曼光谱实际上遵循先前由La hydrids的INS发现的声子态密度(PDOS)。这一方案在“无序”氢化物体系的拉曼散射分析中提出了一个谜,这将被提出和讨论。在CeH2.50中,检测到光谱轮廓从pdos表达的光谱切换到Γ-point-expressed光谱,开始于~ 200 K。在这个温度范围内,晶体场方案的光谱变化,根据嵌入簇计算,被认为是源于八面体H空位的改变。
本文章由计算机程序翻译,如有差异,请以英文原文为准。

Order–Disorder Transitions in Cerium Hydrides, Manifested in Temperature-Dependent Raman Scattering Spectroscopy

Order–Disorder Transitions in Cerium Hydrides, Manifested in Temperature-Dependent Raman Scattering Spectroscopy

Phononic and electronic Raman scattering of CeH2+x (x = 0.25, 0.50, 0.79, and 0.94) were explored within the temperature range of 77–345 K. The experimental analysis was theoretically supported by DFT-calculated phonon dispersion curves and embedded cluster model ab initio calculations of the energies of Ce3+ crystal field states and is correlated with the broadly investigated “twin system” of lanthanide hydrides, which exhibits a highly similar temperature–composition phase diagram. The Raman spectrum of CeH2.94 is dominated by a band with a frequency placed within an energy gap of the calculated phonon dispersion curves of BiF3-type cubic CeH3. This result goes along with structural modification, driven by H displacement from the expected Wyckoff positions, and in particular with the additional orthorhombic phase, which theoretically demonstrated LaH∼3 to be the dynamically stable phase among the two phases. Octahedral H-sublattice rearrangements, strongly affected by repulsive H–H interactions, are known to drive the temperature-dependent order–disorder transformations in lanthanide hydrides. Hydrides with 0.7 < x < 0.8 were previously shown to undergo an electronic (metal–semiconductor) transition at ∼245 K, which is accompanied by a structural (cubic–tetragonal) phase transition. Here, we systematically demonstrate the ability of Raman scattering to closely follow this transition for CeH2.79 by monitoring the tetrahedral H-sublattice phonons, as well as by following changes in the crystal field scheme around the Ce3+ ions. In the lanthanum “twin system” of CeH2.25 and CeH2.50, the structured long-range tetragonal order formed below ∼200 K is manifested in the temperature evolution of its diffraction patterns. However, although first-order Raman scattering spectra of solids with well-defined structures are composed of Brillouin Γ-point symmetry-allowed phonons, the CeH2.25 Raman spectra practically follow the phonon density of states (PDOS), previously found by INS of La hydrides. This scheme raises an enigma in the Raman scattering analysis of “disordered” hydride systems, which will be presented and discussed. In CeH2.50, a switch of the spectral profile is detected from PDOS-expressed spectrum to Γ-point-expressed spectrum commences at ∼200 K. Spectral changes in the crystal field scheme, also found in this temperature range, are argued, according to embedded cluster calculations, to stem from the modified landscape of octahedral H vacancies.

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来源期刊
The Journal of Physical Chemistry C
The Journal of Physical Chemistry C 化学-材料科学:综合
CiteScore
6.50
自引率
8.10%
发文量
2047
审稿时长
1.8 months
期刊介绍: The Journal of Physical Chemistry A/B/C is devoted to reporting new and original experimental and theoretical basic research of interest to physical chemists, biophysical chemists, and chemical physicists.
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