Mechanochemical Synthesis, Structure, and Ionic Conductivity of K2NaYCl6 and KNa2YCl6
K2NaYCl6 and KNa2YCl6 were prepared by a mechanochemical synthesis route from NaCl, KCl, and YCl3 as starting materials. The crystal structures and properties were characterized by X-ray powder diffraction, thermogravimetric and differential thermal analyses, energy-dispersive X-ray spectroscopy, an...
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Veröffentlicht in: | Journal of physical chemistry. C 2024-06, Vol.128 (22), p.8900-8910 |
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creator | Ben Yahia, Hamdi Motohashi, Kota Ishibashi, Hiroki Kubota, Yoshiki Kosuga, Atsuko Sakuda, Atsushi Hayashi, Akitoshi |
description | K2NaYCl6 and KNa2YCl6 were prepared by a mechanochemical synthesis route from NaCl, KCl, and YCl3 as starting materials. The crystal structures and properties were characterized by X-ray powder diffraction, thermogravimetric and differential thermal analyses, energy-dispersive X-ray spectroscopy, and electrochemical impedance spectroscopy. At room temperature, both samples are isostructural to P21/c-Ba2LaRuO6. At high temperature (T < 500 °C), only K2NaYCl6 exhibits a phase transition from the room-temperature form, which crystallizes in the monoclinic system, space group P21/c (No. 14) with a = 7.2447(4) Å, b = 7.5518(4) Å, c = 12.6454(8) Å, β = 124.557(3)°, V = 569.76(6) Å3, and Z = 2 to the high-temperature form, which crystallizes in the cubic system, space group Fm3̅m (No. 225) with a = 10.6903(1) Å, V = 1221.72(1) Å3, and Z = 4. The HT-K2NaYCl6 (cF40) polymorph is isostructural to K2NaAlF6. The structures are monoclinic and cubic double perovskites A2BB′X6 in which the octahedrally coordinated Na and Y atoms are well-ordered at the B and B′ sites, respectively. The A site is occupied by K and K/Na atoms in K2NaYCl6 and KNa2YCl6, respectively. The P21/c ⇄ Fm3̅m phase transition mechanism was accurately determined and is illustrated in a video. K2NaYCl6 and KNa2YCl6 exhibit ionic conductivities of 8 × 10–8 and 4.9 × 10–9 S cm–1 at 75 °C, respectively. |
doi_str_mv | 10.1021/acs.jpcc.4c01413 |
format | Article |
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The crystal structures and properties were characterized by X-ray powder diffraction, thermogravimetric and differential thermal analyses, energy-dispersive X-ray spectroscopy, and electrochemical impedance spectroscopy. At room temperature, both samples are isostructural to P21/c-Ba2LaRuO6. At high temperature (T < 500 °C), only K2NaYCl6 exhibits a phase transition from the room-temperature form, which crystallizes in the monoclinic system, space group P21/c (No. 14) with a = 7.2447(4) Å, b = 7.5518(4) Å, c = 12.6454(8) Å, β = 124.557(3)°, V = 569.76(6) Å3, and Z = 2 to the high-temperature form, which crystallizes in the cubic system, space group Fm3̅m (No. 225) with a = 10.6903(1) Å, V = 1221.72(1) Å3, and Z = 4. The HT-K2NaYCl6 (cF40) polymorph is isostructural to K2NaAlF6. The structures are monoclinic and cubic double perovskites A2BB′X6 in which the octahedrally coordinated Na and Y atoms are well-ordered at the B and B′ sites, respectively. The A site is occupied by K and K/Na atoms in K2NaYCl6 and KNa2YCl6, respectively. The P21/c ⇄ Fm3̅m phase transition mechanism was accurately determined and is illustrated in a video. K2NaYCl6 and KNa2YCl6 exhibit ionic conductivities of 8 × 10–8 and 4.9 × 10–9 S cm–1 at 75 °C, respectively.</description><identifier>ISSN: 1932-7447</identifier><identifier>EISSN: 1932-7455</identifier><identifier>DOI: 10.1021/acs.jpcc.4c01413</identifier><language>eng</language><publisher>American Chemical Society</publisher><subject>C: Energy Conversion and Storage</subject><ispartof>Journal of physical chemistry. C, 2024-06, Vol.128 (22), p.8900-8910</ispartof><rights>2024 American Chemical Society</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><orcidid>0000-0001-9503-5561 ; 0000-0001-6577-9498 ; 0000-0002-9214-0347 ; 0000-0001-9318-7588</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://pubs.acs.org/doi/pdf/10.1021/acs.jpcc.4c01413$$EPDF$$P50$$Gacs$$H</linktopdf><linktohtml>$$Uhttps://pubs.acs.org/doi/10.1021/acs.jpcc.4c01413$$EHTML$$P50$$Gacs$$H</linktohtml><link.rule.ids>314,780,784,27076,27924,27925,56738,56788</link.rule.ids></links><search><creatorcontrib>Ben Yahia, Hamdi</creatorcontrib><creatorcontrib>Motohashi, Kota</creatorcontrib><creatorcontrib>Ishibashi, Hiroki</creatorcontrib><creatorcontrib>Kubota, Yoshiki</creatorcontrib><creatorcontrib>Kosuga, Atsuko</creatorcontrib><creatorcontrib>Sakuda, Atsushi</creatorcontrib><creatorcontrib>Hayashi, Akitoshi</creatorcontrib><title>Mechanochemical Synthesis, Structure, and Ionic Conductivity of K2NaYCl6 and KNa2YCl6</title><title>Journal of physical chemistry. C</title><addtitle>J. Phys. Chem. C</addtitle><description>K2NaYCl6 and KNa2YCl6 were prepared by a mechanochemical synthesis route from NaCl, KCl, and YCl3 as starting materials. The crystal structures and properties were characterized by X-ray powder diffraction, thermogravimetric and differential thermal analyses, energy-dispersive X-ray spectroscopy, and electrochemical impedance spectroscopy. At room temperature, both samples are isostructural to P21/c-Ba2LaRuO6. At high temperature (T < 500 °C), only K2NaYCl6 exhibits a phase transition from the room-temperature form, which crystallizes in the monoclinic system, space group P21/c (No. 14) with a = 7.2447(4) Å, b = 7.5518(4) Å, c = 12.6454(8) Å, β = 124.557(3)°, V = 569.76(6) Å3, and Z = 2 to the high-temperature form, which crystallizes in the cubic system, space group Fm3̅m (No. 225) with a = 10.6903(1) Å, V = 1221.72(1) Å3, and Z = 4. The HT-K2NaYCl6 (cF40) polymorph is isostructural to K2NaAlF6. The structures are monoclinic and cubic double perovskites A2BB′X6 in which the octahedrally coordinated Na and Y atoms are well-ordered at the B and B′ sites, respectively. The A site is occupied by K and K/Na atoms in K2NaYCl6 and KNa2YCl6, respectively. The P21/c ⇄ Fm3̅m phase transition mechanism was accurately determined and is illustrated in a video. K2NaYCl6 and KNa2YCl6 exhibit ionic conductivities of 8 × 10–8 and 4.9 × 10–9 S cm–1 at 75 °C, respectively.</description><subject>C: Energy Conversion and Storage</subject><issn>1932-7447</issn><issn>1932-7455</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2024</creationdate><recordtype>article</recordtype><sourceid/><recordid>eNo9kE9Pg0AQxTdGE2v17nE_AODO7C5lj4b4p2mth9qDJzIsuwGCYICa9NtLa-Np3ry8zOT9GLsHEYFAeCA7RPW3tZGyAhTICzYDIzFcKK0v_7VaXLObYaiF0FKAnLHdm7MltZ0t3VdlqeHbQzuWbqiGgG_Hfm_Hfe8CTm3Bl11bWZ52bTG51U81Hnjn-Qo39Jk28Smy2hAel1t25akZ3N15ztnu-ekjfQ3X7y_L9HEdEiCOIUCiC0y8MLEHj6iML1AieE_ekku0EVInOWJhCIwpSJFxRlmX2zgHreWcBX93p_ZZ3e37dvqWgciOSLKTOSHJzkjkL_w5VY0</recordid><startdate>20240606</startdate><enddate>20240606</enddate><creator>Ben Yahia, Hamdi</creator><creator>Motohashi, Kota</creator><creator>Ishibashi, Hiroki</creator><creator>Kubota, Yoshiki</creator><creator>Kosuga, Atsuko</creator><creator>Sakuda, Atsushi</creator><creator>Hayashi, Akitoshi</creator><general>American Chemical Society</general><scope/><orcidid>https://orcid.org/0000-0001-9503-5561</orcidid><orcidid>https://orcid.org/0000-0001-6577-9498</orcidid><orcidid>https://orcid.org/0000-0002-9214-0347</orcidid><orcidid>https://orcid.org/0000-0001-9318-7588</orcidid></search><sort><creationdate>20240606</creationdate><title>Mechanochemical Synthesis, Structure, and Ionic Conductivity of K2NaYCl6 and KNa2YCl6</title><author>Ben Yahia, Hamdi ; Motohashi, Kota ; Ishibashi, Hiroki ; Kubota, Yoshiki ; Kosuga, Atsuko ; Sakuda, Atsushi ; Hayashi, Akitoshi</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-a122t-1185d28f096f1f2249fd2321ffafcae8590358b22d9a199da4a9e94cebc6b1553</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2024</creationdate><topic>C: Energy Conversion and Storage</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Ben Yahia, Hamdi</creatorcontrib><creatorcontrib>Motohashi, Kota</creatorcontrib><creatorcontrib>Ishibashi, Hiroki</creatorcontrib><creatorcontrib>Kubota, Yoshiki</creatorcontrib><creatorcontrib>Kosuga, Atsuko</creatorcontrib><creatorcontrib>Sakuda, Atsushi</creatorcontrib><creatorcontrib>Hayashi, Akitoshi</creatorcontrib><jtitle>Journal of physical chemistry. C</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Ben Yahia, Hamdi</au><au>Motohashi, Kota</au><au>Ishibashi, Hiroki</au><au>Kubota, Yoshiki</au><au>Kosuga, Atsuko</au><au>Sakuda, Atsushi</au><au>Hayashi, Akitoshi</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Mechanochemical Synthesis, Structure, and Ionic Conductivity of K2NaYCl6 and KNa2YCl6</atitle><jtitle>Journal of physical chemistry. C</jtitle><addtitle>J. Phys. Chem. C</addtitle><date>2024-06-06</date><risdate>2024</risdate><volume>128</volume><issue>22</issue><spage>8900</spage><epage>8910</epage><pages>8900-8910</pages><issn>1932-7447</issn><eissn>1932-7455</eissn><abstract>K2NaYCl6 and KNa2YCl6 were prepared by a mechanochemical synthesis route from NaCl, KCl, and YCl3 as starting materials. The crystal structures and properties were characterized by X-ray powder diffraction, thermogravimetric and differential thermal analyses, energy-dispersive X-ray spectroscopy, and electrochemical impedance spectroscopy. At room temperature, both samples are isostructural to P21/c-Ba2LaRuO6. At high temperature (T < 500 °C), only K2NaYCl6 exhibits a phase transition from the room-temperature form, which crystallizes in the monoclinic system, space group P21/c (No. 14) with a = 7.2447(4) Å, b = 7.5518(4) Å, c = 12.6454(8) Å, β = 124.557(3)°, V = 569.76(6) Å3, and Z = 2 to the high-temperature form, which crystallizes in the cubic system, space group Fm3̅m (No. 225) with a = 10.6903(1) Å, V = 1221.72(1) Å3, and Z = 4. The HT-K2NaYCl6 (cF40) polymorph is isostructural to K2NaAlF6. The structures are monoclinic and cubic double perovskites A2BB′X6 in which the octahedrally coordinated Na and Y atoms are well-ordered at the B and B′ sites, respectively. The A site is occupied by K and K/Na atoms in K2NaYCl6 and KNa2YCl6, respectively. The P21/c ⇄ Fm3̅m phase transition mechanism was accurately determined and is illustrated in a video. K2NaYCl6 and KNa2YCl6 exhibit ionic conductivities of 8 × 10–8 and 4.9 × 10–9 S cm–1 at 75 °C, respectively.</abstract><pub>American Chemical Society</pub><doi>10.1021/acs.jpcc.4c01413</doi><tpages>11</tpages><orcidid>https://orcid.org/0000-0001-9503-5561</orcidid><orcidid>https://orcid.org/0000-0001-6577-9498</orcidid><orcidid>https://orcid.org/0000-0002-9214-0347</orcidid><orcidid>https://orcid.org/0000-0001-9318-7588</orcidid></addata></record> |
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title | Mechanochemical Synthesis, Structure, and Ionic Conductivity of K2NaYCl6 and KNa2YCl6 |
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