<HashMap><database>biostudies-literature</database><scores/><additional><omics_type>Unknown</omics_type><volume>62(49)</volume><submitter>Belik AA</submitter><pubmed_abstract>Dy&lt;sub>2&lt;/sub>CuZnMn&lt;sub>4&lt;/sub>O&lt;sub>12&lt;/sub> perovskite, belonging to the A-site columnar-ordered quadruple perovskite family with the general composition of A&lt;sub>2&lt;/sub>A'A″B&lt;sub>4&lt;/sub>O&lt;sub>12&lt;/sub>, was prepared by a high-pressure, high-temperature method at 6 GPa and 1500 K. Its crystal structure was studied by synchrotron powder X-ray diffraction between 100 and 800 K. The ideal cation distribution (without antisite disorder) was found to be realized within the sensitivity of the synchrotron X-ray diffraction method. Between 100 and 400 K, it crystallizes in space group &lt;i>Pmmn&lt;/i> (no. 59) and has layered charge ordering of Mn&lt;sup>3+&lt;/sup> and Mn&lt;sup>4+&lt;/sup> at the B sites. Above 425 K, it crystallizes in space group &lt;i>P&lt;/i>4&lt;sub>2&lt;/sub>/&lt;i>nmc&lt;/i> (no. 137) with one crystallographic B site and an average Mn&lt;sup>3.5+&lt;/sup> oxidation state. The charge ordering transition (at &lt;i>T&lt;/i>&lt;sub>CO&lt;/sub> = 425 K) appears to be of the second order as no anomalies were found on differential scanning calorimetry curves and temperature dependence of the unit cell volume, and the orthorhombic &lt;i>a&lt;/i> and &lt;i>b&lt;/i> lattice parameters merge gradually. The compound demonstrates anisotropic thermal expansion with the &lt;i>c&lt;/i> lattice parameter decreasing with increasing temperature above 280 K. A ferrimagnetic transition occurs at &lt;i>T&lt;/i>&lt;sub>C&lt;/sub> = 116 K with an additional, gradual rise of magnetic susceptibilities below 45 K, probably due to increases of the ordered moments of the Dy sublattices.</pubmed_abstract><journal>Inorganic chemistry</journal><pagination>20042-20049</pagination><full_dataset_link>https://www.ebi.ac.uk/biostudies/studies/S-EPMC10910486</full_dataset_link><repository>biostudies-literature</repository><pubmed_title>Anisotropic Thermal Expansion and a Second-Order Charge Order Transition in the Ferrimagnetic Dy&lt;sub>2&lt;/sub>CuZnMn&lt;sub>4&lt;/sub>O&lt;sub>12&lt;/sub> Perovskite with Triple A-Site Cation Ordering.</pubmed_title><pmcid>PMC10910486</pmcid><pubmed_authors>Belik AA</pubmed_authors></additional><is_claimable>false</is_claimable><name>Anisotropic Thermal Expansion and a Second-Order Charge Order Transition in the Ferrimagnetic Dy&lt;sub>2&lt;/sub>CuZnMn&lt;sub>4&lt;/sub>O&lt;sub>12&lt;/sub> Perovskite with Triple A-Site Cation Ordering.</name><description>Dy&lt;sub>2&lt;/sub>CuZnMn&lt;sub>4&lt;/sub>O&lt;sub>12&lt;/sub> perovskite, belonging to the A-site columnar-ordered quadruple perovskite family with the general composition of A&lt;sub>2&lt;/sub>A'A″B&lt;sub>4&lt;/sub>O&lt;sub>12&lt;/sub>, was prepared by a high-pressure, high-temperature method at 6 GPa and 1500 K. Its crystal structure was studied by synchrotron powder X-ray diffraction between 100 and 800 K. The ideal cation distribution (without antisite disorder) was found to be realized within the sensitivity of the synchrotron X-ray diffraction method. Between 100 and 400 K, it crystallizes in space group &lt;i>Pmmn&lt;/i> (no. 59) and has layered charge ordering of Mn&lt;sup>3+&lt;/sup> and Mn&lt;sup>4+&lt;/sup> at the B sites. Above 425 K, it crystallizes in space group &lt;i>P&lt;/i>4&lt;sub>2&lt;/sub>/&lt;i>nmc&lt;/i> (no. 137) with one crystallographic B site and an average Mn&lt;sup>3.5+&lt;/sup> oxidation state. The charge ordering transition (at &lt;i>T&lt;/i>&lt;sub>CO&lt;/sub> = 425 K) appears to be of the second order as no anomalies were found on differential scanning calorimetry curves and temperature dependence of the unit cell volume, and the orthorhombic &lt;i>a&lt;/i> and &lt;i>b&lt;/i> lattice parameters merge gradually. The compound demonstrates anisotropic thermal expansion with the &lt;i>c&lt;/i> lattice parameter decreasing with increasing temperature above 280 K. A ferrimagnetic transition occurs at &lt;i>T&lt;/i>&lt;sub>C&lt;/sub> = 116 K with an additional, gradual rise of magnetic susceptibilities below 45 K, probably due to increases of the ordered moments of the Dy sublattices.</description><dates><release>2023-01-01T00:00:00Z</release><publication>2023 Dec</publication><modification>2025-04-05T11:38:55.226Z</modification><creation>2025-04-05T11:38:55.226Z</creation></dates><accession>S-EPMC10910486</accession><cross_references><pubmed>38012860</pubmed><doi>10.1021/acs.inorgchem.3c02835</doi></cross_references></HashMap>