<HashMap><database>biostudies-literature</database><scores/><additional><submitter>Ishtiyak M</submitter><funding>Louisiana State University</funding><funding>Basic Energy Sciences</funding><funding>Louisiana Board of Regents</funding><funding>Division of Materials Research</funding><pagination>20226-20239</pagination><full_dataset_link>https://www.ebi.ac.uk/biostudies/studies/S-EPMC11523219</full_dataset_link><repository>biostudies-literature</repository><omics_type>Unknown</omics_type><volume>63(43)</volume><pubmed_abstract>Two novel quaternary oxyarsenides, Eu&lt;sub>8&lt;/sub>Zn&lt;sub>2&lt;/sub>As&lt;sub>6&lt;/sub>O and Eu&lt;sub>14&lt;/sub>Zn&lt;sub>5&lt;/sub>As&lt;sub>12&lt;/sub>O, were synthesized through metal flux reactions, and their crystal structures were established by single-crystal X-ray diffraction methods. Eu&lt;sub>8&lt;/sub>Zn&lt;sub>2&lt;/sub>As&lt;sub>6&lt;/sub>O crystallizes in the orthorhombic space group &lt;i>Pbca&lt;/i>, featuring polyanionic ribbons composed of corner-shared triangular [ZnAs&lt;sub>3&lt;/sub>] units, running along the [100] direction. The structure of Eu&lt;sub>14&lt;/sub>Zn&lt;sub>5&lt;/sub>As&lt;sub>12&lt;/sub>O crystallizes in the monoclinic space group &lt;i>P&lt;/i>2/&lt;i>m&lt;/i> and its anionic substructure can be described as an infinite "ribbonlike" chain comprised of [ZnAs&lt;sub>3&lt;/sub>] trigonal-planar units, although the structural complexity here is greater and also amplified by disorder on multiple crystallographic positions. In both structures, the O&lt;sup>2-&lt;/sup> anion occupies an octahedral void with six neighboring Eu&lt;sup>2+&lt;/sup> cations. Formal electron counting, electronic structure calculations, and transport properties reveal the charge-balanced semiconducting nature of these heteroanionic Zintl phases. High-temperature thermoelectric transport properties measurements on Eu&lt;sub>14&lt;/sub>Zn&lt;sub>5&lt;/sub>As&lt;sub>12&lt;/sub>O reveal relatively high resistivity (&lt;i>ρ&lt;/i>&lt;sub>500K&lt;/sub> = 8 Ω·cm) and Seebeck coefficient values (&lt;i>S&lt;/i>&lt;sub>500K&lt;/sub> = 220 μV K&lt;sup>-1&lt;/sup>), along with a low concentration and mobility of holes as the dominant charge-carriers (&lt;i>n&lt;/i>&lt;sub&gt;500K&lt;/sub> = 8.0 × 10&lt;sup>17&lt;/sup> cm&lt;sup>-3&lt;/sup>, &lt;i>μ&lt;/i>&lt;sub>500K&lt;/sub> = 6.4 cm&lt;sup>2&lt;/sup>/V s). Magnetic studies indicate the presence of divalent Eu&lt;sup>2+&lt;/sup> species in Eu&lt;sub>14&lt;/sub>Zn&lt;sub>5&lt;/sub>As&lt;sub>12&lt;/sub>O and complex magnetic ordering, with two transitions observed at &lt;i>T&lt;/i>&lt;sub>1&lt;/sub> = 21.6 K and &lt;i>T&lt;/i>&lt;sub>2&lt;/sub> = 9 K.</pubmed_abstract><journal>Inorganic chemistry</journal><pubmed_title>Advancing Heteroanionicity in Zintl Phases: Crystal Structures, Thermoelectric and Magnetic Properties of Two Quaternary Semiconducting Arsenide Oxides, Eu&amp;lt;sub&amp;gt;8&amp;lt;/sub&amp;gt;Zn&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;As&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;O and Eu&amp;lt;sub&amp;gt;14&amp;lt;/sub&amp;gt;Zn&amp;lt;sub&amp;gt;5&amp;lt;/sub&amp;gt;As&amp;lt;sub&amp;gt;12&amp;lt;/sub&amp;gt;O.</pubmed_title><pmcid>PMC11523219</pmcid><funding_grant_id>LEQSF (2024-27)-RD-A-06</funding_grant_id><funding_grant_id>1904636</funding_grant_id><funding_grant_id>DE-SC0008885</funding_grant_id><pubmed_authors>Bobev S</pubmed_authors><pubmed_authors>Ishtiyak M</pubmed_authors><pubmed_authors>Thipe B</pubmed_authors><pubmed_authors>Young DP</pubmed_authors><pubmed_authors>Womack F</pubmed_authors><pubmed_authors>Adams P</pubmed_authors><pubmed_authors>Watts SR</pubmed_authors><pubmed_authors>Bai X</pubmed_authors><pubmed_authors>Baranets S</pubmed_authors></additional><is_claimable>false</is_claimable><name>Advancing Heteroanionicity in Zintl Phases: Crystal Structures, Thermoelectric and Magnetic Properties of Two Quaternary Semiconducting Arsenide Oxides, Eu&amp;lt;sub&amp;gt;8&amp;lt;/sub&amp;gt;Zn&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;As&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;O and Eu&amp;lt;sub&amp;gt;14&amp;lt;/sub&amp;gt;Zn&amp;lt;sub&amp;gt;5&amp;lt;/sub&amp;gt;As&amp;lt;sub&amp;gt;12&amp;lt;/sub&amp;gt;O.</name><description>Two novel quaternary oxyarsenides, Eu&lt;sub>8&lt;/sub>Zn&lt;sub>2&lt;/sub>As&lt;sub>6&lt;/sub>O and Eu&lt;sub>14&lt;/sub>Zn&lt;sub>5&lt;/sub>As&lt;sub>12&lt;/sub>O, were synthesized through metal flux reactions, and their crystal structures were established by single-crystal X-ray diffraction methods. Eu&lt;sub>8&lt;/sub>Zn&lt;sub>2&lt;/sub>As&lt;sub>6&lt;/sub>O crystallizes in the orthorhombic space group &lt;i>Pbca&lt;/i>, featuring polyanionic ribbons composed of corner-shared triangular [ZnAs&lt;sub>3&lt;/sub>] units, running along the [100] direction. The structure of Eu&lt;sub>14&lt;/sub>Zn&lt;sub>5&lt;/sub>As&lt;sub>12&lt;/sub>O crystallizes in the monoclinic space group &lt;i>P&lt;/i>2/&lt;i>m&lt;/i> and its anionic substructure can be described as an infinite "ribbonlike" chain comprised of [ZnAs&lt;sub>3&lt;/sub>] trigonal-planar units, although the structural complexity here is greater and also amplified by disorder on multiple crystallographic positions. In both structures, the O&lt;sup>2-&lt;/sup> anion occupies an octahedral void with six neighboring Eu&lt;sup>2+&lt;/sup> cations. Formal electron counting, electronic structure calculations, and transport properties reveal the charge-balanced semiconducting nature of these heteroanionic Zintl phases. High-temperature thermoelectric transport properties measurements on Eu&lt;sub>14&lt;/sub>Zn&lt;sub>5&lt;/sub>As&lt;sub>12&lt;/sub>O reveal relatively high resistivity (&lt;i>ρ&lt;/i>&lt;sub>500K&lt;/sub> = 8 Ω·cm) and Seebeck coefficient values (&lt;i>S&lt;/i>&lt;sub>500K&lt;/sub> = 220 μV K&lt;sup>-1&lt;/sup>), along with a low concentration and mobility of holes as the dominant charge-carriers (&lt;i>n&lt;/i>&lt;sub&gt;500K&lt;/sub> = 8.0 × 10&lt;sup>17&lt;/sup> cm&lt;sup>-3&lt;/sup>, &lt;i>μ&lt;/i>&lt;sub>500K&lt;/sub> = 6.4 cm&lt;sup>2&lt;/sup>/V s). Magnetic studies indicate the presence of divalent Eu&lt;sup>2+&lt;/sup> species in Eu&lt;sub>14&lt;/sub>Zn&lt;sub>5&lt;/sub>As&lt;sub>12&lt;/sub>O and complex magnetic ordering, with two transitions observed at &lt;i>T&lt;/i>&lt;sub>1&lt;/sub> = 21.6 K and &lt;i>T&lt;/i>&lt;sub>2&lt;/sub> = 9 K.</description><dates><release>2024-01-01T00:00:00Z</release><publication>2024 Oct</publication><modification>2025-04-04T01:02:37.813Z</modification><creation>2025-04-04T01:02:37.813Z</creation></dates><accession>S-EPMC11523219</accession><cross_references><pubmed>38904454</pubmed><doi>10.1021/acs.inorgchem.4c01580</doi></cross_references></HashMap>