Shahar Aziza, Soshi Iimura, Chengyu Jin, Karin Fink, Shmuel Hayun* and Tsachi Livneh*,
{"title":"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","authors":"Shahar Aziza, Soshi Iimura, Chengyu Jin, Karin Fink, Shmuel Hayun* and Tsachi Livneh*, ","doi":"10.1021/acs.jpcc.5c04145","DOIUrl":null,"url":null,"abstract":"<p >Phononic and electronic Raman scattering of CeH<sub>2+<i>x</i></sub> (<i>x</i> = 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 Ce<sup>3+</sup> 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 CeH<sub>2.94</sub> is dominated by a band with a frequency placed within an energy gap of the calculated phonon dispersion curves of BiF<sub>3</sub>-type cubic CeH<sub>3</sub>. 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<sub>∼3</sub> 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 < <i>x</i> < 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 CeH<sub>2.79</sub> by monitoring the tetrahedral H-sublattice phonons, as well as by following changes in the crystal field scheme around the Ce<sup>3+</sup> ions. In the lanthanum “twin system” of CeH<sub>2.25</sub> and CeH<sub>2.50</sub>, 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 CeH<sub>2.25</sub> 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 CeH<sub>2.50</sub>, 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.</p>","PeriodicalId":61,"journal":{"name":"The Journal of Physical Chemistry C","volume":"129 37","pages":"16826–16843"},"PeriodicalIF":3.2000,"publicationDate":"2025-09-08","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Order–Disorder Transitions in Cerium Hydrides, Manifested in Temperature-Dependent Raman Scattering Spectroscopy\",\"authors\":\"Shahar Aziza, Soshi Iimura, Chengyu Jin, Karin Fink, Shmuel Hayun* and Tsachi Livneh*, \",\"doi\":\"10.1021/acs.jpcc.5c04145\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<p >Phononic and electronic Raman scattering of CeH<sub>2+<i>x</i></sub> (<i>x</i> = 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 Ce<sup>3+</sup> 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 CeH<sub>2.94</sub> is dominated by a band with a frequency placed within an energy gap of the calculated phonon dispersion curves of BiF<sub>3</sub>-type cubic CeH<sub>3</sub>. 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<sub>∼3</sub> 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 < <i>x</i> < 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 CeH<sub>2.79</sub> by monitoring the tetrahedral H-sublattice phonons, as well as by following changes in the crystal field scheme around the Ce<sup>3+</sup> ions. In the lanthanum “twin system” of CeH<sub>2.25</sub> and CeH<sub>2.50</sub>, 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 CeH<sub>2.25</sub> 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 CeH<sub>2.50</sub>, 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.</p>\",\"PeriodicalId\":61,\"journal\":{\"name\":\"The Journal of Physical Chemistry C\",\"volume\":\"129 37\",\"pages\":\"16826–16843\"},\"PeriodicalIF\":3.2000,\"publicationDate\":\"2025-09-08\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"The Journal of Physical Chemistry C\",\"FirstCategoryId\":\"1\",\"ListUrlMain\":\"https://pubs.acs.org/doi/10.1021/acs.jpcc.5c04145\",\"RegionNum\":3,\"RegionCategory\":\"化学\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q2\",\"JCRName\":\"CHEMISTRY, PHYSICAL\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"The Journal of Physical Chemistry C","FirstCategoryId":"1","ListUrlMain":"https://pubs.acs.org/doi/10.1021/acs.jpcc.5c04145","RegionNum":3,"RegionCategory":"化学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"CHEMISTRY, PHYSICAL","Score":null,"Total":0}
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.
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.