Rare-Earth Metal Compounds (2nd Edition)

A special issue of Crystals (ISSN 2073-4352). This special issue belongs to the section "Inorganic Crystalline Materials".

Deadline for manuscript submissions: closed (30 September 2023) | Viewed by 2285

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Institute for Inorganic Chemistry, University of Stuttgart, 70569 Stuttgart, Germany
Interests: rare-earth metal compounds with mixed anions; luminescent materials; compounds with lone-pair oxoanions; hydroborates; thermoanalysis and phase and structure elucidation via X-ray diffraction
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Dear Colleagues,

"These elements perplex us in our researches, baffle us in our speculations, and haunt us in our very dreams. They stretch like an unknown sea before us—mocking, mystifying, and murmuring strange revelations and possibilities" (Sir William Crookes, 1887). These words—135 years old, but still true—are from a rare-earth metal pioneer, who contributed greatly to the commercialization of science. "The Fraternal Fifteen" (Ln = La + Ce-Lu), as "mister rare earth" Karl A. Gschneidner, Jr., called the most similar of them in his 1966 book, were brought to a broader public in the 20th century, emphasizing their benefits to mankind. Even now, when it is more common knowledge that the rare earths are “Neither Rare, Nor Earths" (RE = Sc, Y, La + Ce – Lu) (BBC World Service (2014)), we encourage authors in the field to contribute to this Special Issue of Crystals with the crystal structures and properties of rare-earth metal compounds for readers in both academia and industry.

Prof. Dr. Thomas Schleid
Guest Editor

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16 pages, 2744 KiB  
Article
Synthesis, Crystal Structure and Properties of the New Laminar Quaternary Tellurides SrLnCuTe3 (Ln = Sm, Gd–Tm and Lu)
by Anna V. Ruseikina, Maxim V. Grigoriev, Maxim S. Molokeev, Alexander A. Garmonov, Andrey V. Elyshev, Ralf J. C. Locke and Thomas Schleid
Crystals 2023, 13(2), 291; https://doi.org/10.3390/cryst13020291 - 9 Feb 2023
Cited by 4 | Viewed by 1690
Abstract
This paper reports for the first time on the new laminar quaternary orthorhombic heterometallic quaternary tellurides SrLnCuTe3, the fabrication of which has been a challenge until this work. Data on the crystal structure of tellurides complete the series of [...] Read more.
This paper reports for the first time on the new laminar quaternary orthorhombic heterometallic quaternary tellurides SrLnCuTe3, the fabrication of which has been a challenge until this work. Data on the crystal structure of tellurides complete the series of quaternary strontium chalcogenides SrLnCuCh3 (Ch = S, Se, Te). Single crystals of the compounds were synthesized from the elements by the halogenide-flux method at 1070 K. The compounds are crystallizing in two space groups Pnma (Ln = Sm, Gd and Tb) and Cmcm (Ln = Dy–Tm and Lu). For SrSmCuTe3 (a = 11.4592(7), b = 4.3706(3), c = 14.4425(9) Å, space group: Pnma) with the largest lanthanoid cation, Sr2+ shows C.N. = 7, whereas Sm3+ reveals a diminished coordination number C.N. = 6. For SrLuCuTe3 (a = 4.3064(3), b = 14.3879(9), c = 11.1408(7) Å, space group: Cmcm) with the smallest lanthanoid cation, coordination numbers of six are realized for both high-charged cations (Sr2+ and Lu3+: C.N. = 6). The cations Sr2+, Ln3+, Cu+ each take independent positions. The structures are built by distorted [CuTe4]7– tetrahedra, forming the infinite chains {1[Cu(Te1)1/1t(Te2)1/1t(Te3)2/2e]5} along [010] in SrLnCuTe3 (Ln = Sm, Gd and Tb) and [100] in SrLnCuTe3 (Ln = Dy–Tm and Lu). The distortion of the polyhedra [CuTe4]7– was compared for the whole series SrLnCuTe3 by means of τ4-descriptor for the four coordinating Te2– anions, which revealed a decrease in the degree of distortion with a decreasing radius at Ln3+. The distorted octahedra [LnTe6]9– form layers {2[Ln(Te1)2/2(Te2)2/2(Te3)2/2]3}. The distorted octahedra and tetrahedra fuse to form parallel layers {2[CuLnTe3]2} and between them, the Sr2+ cations providing three-dimensionality of the structure are located. In the SrLnCuTe3 (Ln = Sm, Gd and Tb) structures, the Sr2+ cations center capped the trigonal prisms [SrTe6+1]12−, united in infinite chains {1[Sr(Te1)2/2(Te2)3/3(Te3)2/2]4} along the [100] direction. The domains of existence of the Ba2MnS3, BaLaCuS3, Eu2CuS3 and KZrCuS3 structure types are defined in the series of orthorhombic chalcogenides SrLnCuCh3 (Ch = S, Se and Te). The tellurides SrLnCuTe3 (Ln = Tb–Er) of both structure types in the temperature range from 2 up to 300 K are paramagnetic, without showing clear signs of a magnetic phase transition. Full article
(This article belongs to the Special Issue Rare-Earth Metal Compounds (2nd Edition))
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