氟化镧系元素(III)氧化砷酸盐(III)Ln 5F3[AsO3]4(Ln = Eu-Lu)的同种型系列

Ralf J. C. Locke, Florian Ledderboge, Felix C. Goerigk, Frank C. Zimmer, Thomas Schleid
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They all crystallize tetragonally in the space group <jats:italic>P</jats:italic>4/<jats:italic>ncc</jats:italic> with lattice parameters ranging from <jats:italic>a</jats:italic> = 1164.71(8) pm and <jats:italic>c</jats:italic> = 1097.95(7) pm for Eu<jats:sub>5</jats:sub>F<jats:sub>3</jats:sub>[AsO<jats:sub>4</jats:sub>]<jats:sub>4</jats:sub> down to <jats:italic>a</jats:italic> = 1125.72(8) pm and <jats:italic>c</jats:italic> = 1061.16(7) pm for Lu<jats:sub>5</jats:sub>F<jats:sub>3</jats:sub>[AsO<jats:sub>3</jats:sub>]<jats:sub>4</jats:sub> for <jats:italic>Z</jats:italic> = 4 as consequence of the lanthanoid contraction. The crystal structure exhibits three positions for the trications occupied by one As<jats:sup>3+</jats:sup> and two <jats:italic>Ln</jats:italic> <jats:sup>3+</jats:sup> species. The lanthanoids occur with two different coordination polyhedra consisting of a fluoride-capped oxygen cube [(<jats:italic>Ln</jats:italic>1)O<jats:sub>8</jats:sub>F]<jats:sup>14−</jats:sup> and a bicapped trigonal prism [(<jats:italic>Ln</jats:italic>2)O<jats:sub>6</jats:sub>F<jats:sub>2</jats:sub>]<jats:sup>11−</jats:sup> of F<jats:sup>−</jats:sup> and O<jats:sup>2−</jats:sup> anions. A surprisingly diverse <jats:italic>Ln</jats:italic> <jats:sup>3+</jats:sup> cation coordination for the F<jats:sup>−</jats:sup> anions is noteworthy, as (F1)<jats:sup>−</jats:sup> has contact to five, but (F2)<jats:sup>−</jats:sup> to only two of them. The crystallographically unique As<jats:sup>3+</jats:sup> cation is coordinated in a discrete <jats:italic>ψ</jats:italic> <jats:sup>1</jats:sup>-tetrahedron [AsO<jats:sub>3</jats:sub>]<jats:sup>3−</jats:sup> by three oxygen atoms. The lone-pairs of electrons at the As<jats:sup>3+</jats:sup> centers point into empty channels along [001], flanked by four columns of condensed [(<jats:italic>Ln</jats:italic>1)O<jats:sub>8</jats:sub>F]<jats:sup>14−</jats:sup> polyhedra. As rather short oxygen-fluorine distances are present within this structural feature, the absence of (OH)<jats:sup>−</jats:sup> units apt to replace F<jats:sup>−</jats:sup> needed to be verified by single-crystal Raman spectroscopy. The composition <jats:italic>Ln</jats:italic> <jats:sub>5</jats:sub>F<jats:sub>3</jats:sub>[AsO<jats:sub>3</jats:sub>] was also confirmed by electron-beam microprobe (EDXS) measurements and the phase purity of selected samples could be proven by powder X-ray diffractometry (PXRD).","PeriodicalId":23831,"journal":{"name":"Zeitschrift für Naturforschung B","volume":"26 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2024-06-27","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"The isotypic series of tetragonal lanthanoid(III) fluoride oxoarsenates(III) Ln 5F3[AsO3]4 (Ln = Eu–Lu)\",\"authors\":\"Ralf J. C. Locke, Florian Ledderboge, Felix C. Goerigk, Frank C. Zimmer, Thomas Schleid\",\"doi\":\"10.1515/znb-2024-0030\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"The new fluoride-containing lanthanoid(III) oxoarsenates(III) with the composition <jats:italic>Ln</jats:italic> <jats:sub>5</jats:sub>F<jats:sub>3</jats:sub>[AsO<jats:sub>3</jats:sub>]<jats:sub>4</jats:sub> (<jats:italic>Ln</jats:italic> = Eu–Lu) could be obtained through partial metallothermic reduction from mixtures of the corresponding trifluorides (<jats:italic>Ln</jats:italic>F<jats:sub>3</jats:sub>) and the metals (<jats:italic>Ln</jats:italic>) with As<jats:sub>2</jats:sub>O<jats:sub>3</jats:sub> upon heating in fused silica ampoules. They all crystallize tetragonally in the space group <jats:italic>P</jats:italic>4/<jats:italic>ncc</jats:italic> with lattice parameters ranging from <jats:italic>a</jats:italic> = 1164.71(8) pm and <jats:italic>c</jats:italic> = 1097.95(7) pm for Eu<jats:sub>5</jats:sub>F<jats:sub>3</jats:sub>[AsO<jats:sub>4</jats:sub>]<jats:sub>4</jats:sub> down to <jats:italic>a</jats:italic> = 1125.72(8) pm and <jats:italic>c</jats:italic> = 1061.16(7) pm for Lu<jats:sub>5</jats:sub>F<jats:sub>3</jats:sub>[AsO<jats:sub>3</jats:sub>]<jats:sub>4</jats:sub> for <jats:italic>Z</jats:italic> = 4 as consequence of the lanthanoid contraction. The crystal structure exhibits three positions for the trications occupied by one As<jats:sup>3+</jats:sup> and two <jats:italic>Ln</jats:italic> <jats:sup>3+</jats:sup> species. The lanthanoids occur with two different coordination polyhedra consisting of a fluoride-capped oxygen cube [(<jats:italic>Ln</jats:italic>1)O<jats:sub>8</jats:sub>F]<jats:sup>14−</jats:sup> and a bicapped trigonal prism [(<jats:italic>Ln</jats:italic>2)O<jats:sub>6</jats:sub>F<jats:sub>2</jats:sub>]<jats:sup>11−</jats:sup> of F<jats:sup>−</jats:sup> and O<jats:sup>2−</jats:sup> anions. A surprisingly diverse <jats:italic>Ln</jats:italic> <jats:sup>3+</jats:sup> cation coordination for the F<jats:sup>−</jats:sup> anions is noteworthy, as (F1)<jats:sup>−</jats:sup> has contact to five, but (F2)<jats:sup>−</jats:sup> to only two of them. The crystallographically unique As<jats:sup>3+</jats:sup> cation is coordinated in a discrete <jats:italic>ψ</jats:italic> <jats:sup>1</jats:sup>-tetrahedron [AsO<jats:sub>3</jats:sub>]<jats:sup>3−</jats:sup> by three oxygen atoms. The lone-pairs of electrons at the As<jats:sup>3+</jats:sup> centers point into empty channels along [001], flanked by four columns of condensed [(<jats:italic>Ln</jats:italic>1)O<jats:sub>8</jats:sub>F]<jats:sup>14−</jats:sup> polyhedra. As rather short oxygen-fluorine distances are present within this structural feature, the absence of (OH)<jats:sup>−</jats:sup> units apt to replace F<jats:sup>−</jats:sup> needed to be verified by single-crystal Raman spectroscopy. The composition <jats:italic>Ln</jats:italic> <jats:sub>5</jats:sub>F<jats:sub>3</jats:sub>[AsO<jats:sub>3</jats:sub>] was also confirmed by electron-beam microprobe (EDXS) measurements and the phase purity of selected samples could be proven by powder X-ray diffractometry (PXRD).\",\"PeriodicalId\":23831,\"journal\":{\"name\":\"Zeitschrift für Naturforschung B\",\"volume\":\"26 1\",\"pages\":\"\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2024-06-27\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Zeitschrift für Naturforschung B\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1515/znb-2024-0030\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Zeitschrift für Naturforschung B","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1515/znb-2024-0030","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
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摘要

在熔融石英安瓿瓶中加热相应的三氟化物(LnF3)和金属(Ln)与 As2O3 的混合物,通过部分金属热还原法可获得成分为 Ln 5F3[AsO3]4(Ln = Eu-Lu)的新型含氟镧系(III)氧胂酸盐(III)。它们都在空间群 P4/ncc 中呈四边形结晶,晶格参数从 Eu5F3[AsO4]4 的 a = 1164.71(8) pm 和 c = 1097.95(7) pm 到 Z = 4 的 Lu5F3[AsO3]4 的 a = 1125.72(8) pm 和 c = 1061.16(7) pm 不等,这是镧系收缩的结果。晶体结构显示了由一个 As3+ 和两个 Ln 3+ 物种占据的三个位置。镧系元素具有两种不同的配位多面体,包括一个氟化物封顶的氧立方体[(Ln1)O8F]14-和一个由 F- 和 O2- 阴离子组成的双封顶三棱柱[(Ln2)O6F2]11-。值得注意的是,F- 阴离子的 Ln 3+ 阳离子配位具有惊人的多样性,(F1)- 与五个阳离子接触,但 (F2)- 仅与其中两个阳离子接触。晶体学上独特的 As3+ 阳离子在离散的 ψ 1 四面体 [AsO3]3- 中与三个氧原子配位。As3+ 中心的孤电子对沿着 [001] 指向空通道,两侧是四列缩合的 [(Ln1)O8F]14-多面体。由于这一结构特征中的氧氟距离很短,因此需要通过单晶拉曼光谱来验证是否存在可替代 F- 的 (OH)- 单元。电子束微探针(EDXS)测量也证实了 Ln 5F3[AsO3] 的组成,粉末 X 射线衍射仪(PXRD)也证明了所选样品的相纯度。
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The isotypic series of tetragonal lanthanoid(III) fluoride oxoarsenates(III) Ln 5F3[AsO3]4 (Ln = Eu–Lu)
The new fluoride-containing lanthanoid(III) oxoarsenates(III) with the composition Ln 5F3[AsO3]4 (Ln = Eu–Lu) could be obtained through partial metallothermic reduction from mixtures of the corresponding trifluorides (LnF3) and the metals (Ln) with As2O3 upon heating in fused silica ampoules. They all crystallize tetragonally in the space group P4/ncc with lattice parameters ranging from a = 1164.71(8) pm and c = 1097.95(7) pm for Eu5F3[AsO4]4 down to a = 1125.72(8) pm and c = 1061.16(7) pm for Lu5F3[AsO3]4 for Z = 4 as consequence of the lanthanoid contraction. The crystal structure exhibits three positions for the trications occupied by one As3+ and two Ln 3+ species. The lanthanoids occur with two different coordination polyhedra consisting of a fluoride-capped oxygen cube [(Ln1)O8F]14− and a bicapped trigonal prism [(Ln2)O6F2]11− of F and O2− anions. A surprisingly diverse Ln 3+ cation coordination for the F anions is noteworthy, as (F1) has contact to five, but (F2) to only two of them. The crystallographically unique As3+ cation is coordinated in a discrete ψ 1-tetrahedron [AsO3]3− by three oxygen atoms. The lone-pairs of electrons at the As3+ centers point into empty channels along [001], flanked by four columns of condensed [(Ln1)O8F]14− polyhedra. As rather short oxygen-fluorine distances are present within this structural feature, the absence of (OH) units apt to replace F needed to be verified by single-crystal Raman spectroscopy. The composition Ln 5F3[AsO3] was also confirmed by electron-beam microprobe (EDXS) measurements and the phase purity of selected samples could be proven by powder X-ray diffractometry (PXRD).
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