Crystallography at non-ambient conditions and physical properties of the synthesized double perovskites, Sr2(Co1−xFex)TeO6
Polycrystalline double perovskite-type Sr2(Co1−xFex)TeO6 with various stoichiometric compositions (x = 0, 0.25, 0.5, 0.75, and 1) were synthesized by solid-state reactions in air. The crystal structures and phase transitions of this series at different temperature intervals were determined by X-ray...
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Veröffentlicht in: | Dalton transactions : an international journal of inorganic chemistry 2023-03, Vol.52 (13), p.4086-4102 |
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description | Polycrystalline double perovskite-type Sr2(Co1−xFex)TeO6 with various stoichiometric compositions (x = 0, 0.25, 0.5, 0.75, and 1) were synthesized by solid-state reactions in air. The crystal structures and phase transitions of this series at different temperature intervals were determined by X-ray powder diffraction, and from the obtained data the crystal structures were refined. It has been proven that for the compositions x = 0.25, 0.50, and 0.75, the phases crystallize at room temperature in the monoclinic space group I2/m. Down to 100 K, depending on the composition, these structures experience a phase transition from I2/m to P21/n. At high temperatures up to 1100 K their crystal structures show two further phase transitions. The first one is a first-order phase transition, from monoclinic I2/m to tetragonal I4/m, followed by a second-order phase transition to cubic Fm3m. Therefore, the phase transition sequence of this series detected at temperatures ranging from 100 K to 1100 K is P21/n → I2/m → I4/m → Fm3m. The temperature-dependent vibrational features of the octahedral sites were investigated by Raman spectroscopy, which furthermore complements the XRD results. A decrease in the phase-transition temperature with increasing iron content has been observed for these compounds. This fact is explained by the progressive diminishing of the distortion of the double-perovskite structure in this series. Using room-temperature Mössbauer spectroscopy, the presence of two iron sites is confirmed. The two different transition metal cations Co and Fe at the B sites allow exploring their effect on the optical band-gap. |
doi_str_mv | 10.1039/d2dt03543j |
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The crystal structures and phase transitions of this series at different temperature intervals were determined by X-ray powder diffraction, and from the obtained data the crystal structures were refined. It has been proven that for the compositions x = 0.25, 0.50, and 0.75, the phases crystallize at room temperature in the monoclinic space group I2/m. Down to 100 K, depending on the composition, these structures experience a phase transition from I2/m to P21/n. At high temperatures up to 1100 K their crystal structures show two further phase transitions. The first one is a first-order phase transition, from monoclinic I2/m to tetragonal I4/m, followed by a second-order phase transition to cubic Fm3m. Therefore, the phase transition sequence of this series detected at temperatures ranging from 100 K to 1100 K is P21/n → I2/m → I4/m → Fm3m. The temperature-dependent vibrational features of the octahedral sites were investigated by Raman spectroscopy, which furthermore complements the XRD results. A decrease in the phase-transition temperature with increasing iron content has been observed for these compounds. This fact is explained by the progressive diminishing of the distortion of the double-perovskite structure in this series. Using room-temperature Mössbauer spectroscopy, the presence of two iron sites is confirmed. The two different transition metal cations Co and Fe at the B sites allow exploring their effect on the optical band-gap.</description><identifier>ISSN: 1477-9226</identifier><identifier>EISSN: 1477-9234</identifier><identifier>DOI: 10.1039/d2dt03543j</identifier><language>eng</language><publisher>Cambridge: Royal Society of Chemistry</publisher><subject>Chemical synthesis ; Composition ; Crystal structure ; Crystallography ; High temperature ; Iron ; Monoclinic lattice ; Mossbauer spectroscopy ; Perovskite structure ; Perovskites ; Phase transitions ; Physical properties ; Raman spectroscopy ; Room temperature ; Spectrum analysis ; Temperature ; Temperature dependence ; Transition metals ; Transition temperature ; X ray powder diffraction</subject><ispartof>Dalton transactions : an international journal of inorganic chemistry, 2023-03, Vol.52 (13), p.4086-4102</ispartof><rights>Copyright Royal Society of Chemistry 2023</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,776,780,27901,27902</link.rule.ids></links><search><creatorcontrib>Zaraq, Asmaa</creatorcontrib><creatorcontrib>Orayech, Brahim</creatorcontrib><creatorcontrib>Igartua, Josu M</creatorcontrib><creatorcontrib>Abdeslam El Bouari</creatorcontrib><creatorcontrib>Gregory, Duncan H</creatorcontrib><creatorcontrib>Gesing, Thorsten M</creatorcontrib><title>Crystallography at non-ambient conditions and physical properties of the synthesized double perovskites, Sr2(Co1−xFex)TeO6</title><title>Dalton transactions : an international journal of inorganic chemistry</title><description>Polycrystalline double perovskite-type Sr2(Co1−xFex)TeO6 with various stoichiometric compositions (x = 0, 0.25, 0.5, 0.75, and 1) were synthesized by solid-state reactions in air. The crystal structures and phase transitions of this series at different temperature intervals were determined by X-ray powder diffraction, and from the obtained data the crystal structures were refined. It has been proven that for the compositions x = 0.25, 0.50, and 0.75, the phases crystallize at room temperature in the monoclinic space group I2/m. Down to 100 K, depending on the composition, these structures experience a phase transition from I2/m to P21/n. At high temperatures up to 1100 K their crystal structures show two further phase transitions. The first one is a first-order phase transition, from monoclinic I2/m to tetragonal I4/m, followed by a second-order phase transition to cubic Fm3m. Therefore, the phase transition sequence of this series detected at temperatures ranging from 100 K to 1100 K is P21/n → I2/m → I4/m → Fm3m. The temperature-dependent vibrational features of the octahedral sites were investigated by Raman spectroscopy, which furthermore complements the XRD results. A decrease in the phase-transition temperature with increasing iron content has been observed for these compounds. This fact is explained by the progressive diminishing of the distortion of the double-perovskite structure in this series. Using room-temperature Mössbauer spectroscopy, the presence of two iron sites is confirmed. The two different transition metal cations Co and Fe at the B sites allow exploring their effect on the optical band-gap.</description><subject>Chemical synthesis</subject><subject>Composition</subject><subject>Crystal structure</subject><subject>Crystallography</subject><subject>High temperature</subject><subject>Iron</subject><subject>Monoclinic lattice</subject><subject>Mossbauer spectroscopy</subject><subject>Perovskite structure</subject><subject>Perovskites</subject><subject>Phase transitions</subject><subject>Physical properties</subject><subject>Raman spectroscopy</subject><subject>Room temperature</subject><subject>Spectrum analysis</subject><subject>Temperature</subject><subject>Temperature dependence</subject><subject>Transition metals</subject><subject>Transition temperature</subject><subject>X ray powder diffraction</subject><issn>1477-9226</issn><issn>1477-9234</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2023</creationdate><recordtype>article</recordtype><recordid>eNpdj81KxDAcxIMouK5efIKAlxWs5qNpm6MUV4WFPbiel7T5183aTWqTyq74AJ59RJ_EgOJBGJg5_BhmEDql5JISLq8004FwkfL1HhrRNM8TyXi6_5dZdoiOvF8TwhgRbITey37ng2pb99SrbrXDKmDrbKI2lQEbcO2sNsE467GyGkfCm1q1uOtdB30w4LFrcFgB9jsbzZs30Fi7oWoBR8K9-mcTwF_gh55NSke_Pj63U9ieL2CeHaODRrUeTn59jB6nN4vyLpnNb-_L61nSMZqFpEglFHnKWZ2TXBBZV7yWgvAKNANgIiONAtWoghYkl1UDWohUFU28W6lMSD5Gk5_euPplAB-WG-NraFtlwQ1-yfIi5VEZjejZP3Ttht7GdZGSVBAW-_g3eblv9Q</recordid><startdate>20230328</startdate><enddate>20230328</enddate><creator>Zaraq, Asmaa</creator><creator>Orayech, Brahim</creator><creator>Igartua, Josu M</creator><creator>Abdeslam El Bouari</creator><creator>Gregory, Duncan H</creator><creator>Gesing, Thorsten M</creator><general>Royal Society of Chemistry</general><scope>7SR</scope><scope>7U5</scope><scope>8BQ</scope><scope>8FD</scope><scope>JG9</scope><scope>L7M</scope><scope>7X8</scope></search><sort><creationdate>20230328</creationdate><title>Crystallography at non-ambient conditions and physical properties of the synthesized double perovskites, Sr2(Co1−xFex)TeO6</title><author>Zaraq, Asmaa ; Orayech, Brahim ; Igartua, Josu M ; Abdeslam El Bouari ; Gregory, Duncan H ; Gesing, Thorsten M</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-p216t-849e87432c707509cb3c9503bed2ee2560faeafa818079bfed554a8f922ba6593</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2023</creationdate><topic>Chemical synthesis</topic><topic>Composition</topic><topic>Crystal structure</topic><topic>Crystallography</topic><topic>High temperature</topic><topic>Iron</topic><topic>Monoclinic lattice</topic><topic>Mossbauer spectroscopy</topic><topic>Perovskite structure</topic><topic>Perovskites</topic><topic>Phase transitions</topic><topic>Physical properties</topic><topic>Raman spectroscopy</topic><topic>Room temperature</topic><topic>Spectrum analysis</topic><topic>Temperature</topic><topic>Temperature dependence</topic><topic>Transition metals</topic><topic>Transition temperature</topic><topic>X ray powder diffraction</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Zaraq, Asmaa</creatorcontrib><creatorcontrib>Orayech, Brahim</creatorcontrib><creatorcontrib>Igartua, Josu M</creatorcontrib><creatorcontrib>Abdeslam El Bouari</creatorcontrib><creatorcontrib>Gregory, Duncan H</creatorcontrib><creatorcontrib>Gesing, Thorsten M</creatorcontrib><collection>Engineered Materials Abstracts</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>METADEX</collection><collection>Technology Research Database</collection><collection>Materials Research Database</collection><collection>Advanced Technologies Database with Aerospace</collection><collection>MEDLINE - Academic</collection><jtitle>Dalton transactions : an international journal of inorganic chemistry</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Zaraq, Asmaa</au><au>Orayech, Brahim</au><au>Igartua, Josu M</au><au>Abdeslam El Bouari</au><au>Gregory, Duncan H</au><au>Gesing, Thorsten M</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Crystallography at non-ambient conditions and physical properties of the synthesized double perovskites, Sr2(Co1−xFex)TeO6</atitle><jtitle>Dalton transactions : an international journal of inorganic chemistry</jtitle><date>2023-03-28</date><risdate>2023</risdate><volume>52</volume><issue>13</issue><spage>4086</spage><epage>4102</epage><pages>4086-4102</pages><issn>1477-9226</issn><eissn>1477-9234</eissn><abstract>Polycrystalline double perovskite-type Sr2(Co1−xFex)TeO6 with various stoichiometric compositions (x = 0, 0.25, 0.5, 0.75, and 1) were synthesized by solid-state reactions in air. The crystal structures and phase transitions of this series at different temperature intervals were determined by X-ray powder diffraction, and from the obtained data the crystal structures were refined. It has been proven that for the compositions x = 0.25, 0.50, and 0.75, the phases crystallize at room temperature in the monoclinic space group I2/m. Down to 100 K, depending on the composition, these structures experience a phase transition from I2/m to P21/n. At high temperatures up to 1100 K their crystal structures show two further phase transitions. The first one is a first-order phase transition, from monoclinic I2/m to tetragonal I4/m, followed by a second-order phase transition to cubic Fm3m. Therefore, the phase transition sequence of this series detected at temperatures ranging from 100 K to 1100 K is P21/n → I2/m → I4/m → Fm3m. The temperature-dependent vibrational features of the octahedral sites were investigated by Raman spectroscopy, which furthermore complements the XRD results. A decrease in the phase-transition temperature with increasing iron content has been observed for these compounds. This fact is explained by the progressive diminishing of the distortion of the double-perovskite structure in this series. Using room-temperature Mössbauer spectroscopy, the presence of two iron sites is confirmed. The two different transition metal cations Co and Fe at the B sites allow exploring their effect on the optical band-gap.</abstract><cop>Cambridge</cop><pub>Royal Society of Chemistry</pub><doi>10.1039/d2dt03543j</doi><tpages>17</tpages></addata></record> |
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subjects | Chemical synthesis Composition Crystal structure Crystallography High temperature Iron Monoclinic lattice Mossbauer spectroscopy Perovskite structure Perovskites Phase transitions Physical properties Raman spectroscopy Room temperature Spectrum analysis Temperature Temperature dependence Transition metals Transition temperature X ray powder diffraction |
title | Crystallography at non-ambient conditions and physical properties of the synthesized double perovskites, Sr2(Co1−xFex)TeO6 |
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