Grace Xiong , Ara Jo , Louis S. Wang , Sossina M. Haile
{"title":"Cs2(HSeO4)(H2PO4)中的高温相变和超质子电导率","authors":"Grace Xiong , Ara Jo , Louis S. Wang , Sossina M. Haile","doi":"10.1016/j.ssi.2024.116690","DOIUrl":null,"url":null,"abstract":"<div><p>The compound Cs<sub>2</sub>(HSeO<sub>4</sub>)(H<sub>2</sub>PO<sub>4</sub>) is of interest due to its high conductivity in its superprotonic state. In the present work, in situ X-ray diffraction studies, simultaneous thermal analysis, and AC impedance spectroscopy, each performed under controlled value of steam partial pressure (<em>p</em>H<sub>2</sub>O), were carried out to elucidate the crystallographic features of the transformation and resolve the conductivity in the high temperature phase. The studies reveal that the material transforms to a cubic phase at a temperature of approximately 116 °C, that the activation energy for proton transport in the cubic phase is 0.304(2) eV, and the magnitude of the conductivity is comparable to that of Cs<sub>2</sub>(HSO<sub>4</sub>)(H<sub>2</sub>PO<sub>4</sub>). Despite differences in the room temperature structures of Cs<sub>2</sub>(HSeO<sub>4</sub>)(H<sub>2</sub>PO<sub>4</sub>), Cs<sub>2</sub>(HSO<sub>4</sub>)(H<sub>2</sub>PO<sub>4</sub>), and CsH<sub>2</sub>PO<sub>4</sub>, each has a monoclinic to cubic transformation entropy of approximately 23 J/mol(CsH<sub>x</sub>XO<sub>4</sub>)/K. Under <em>p</em>H<sub>2</sub>O = 0.05 atm, the cubic phase of Cs<sub>2</sub>(HSeO<sub>4</sub>)(H<sub>2</sub>PO<sub>4</sub>) is stable to approximately 250 °C. Under elevated <em>p</em>H<sub>2</sub>O (0.3 atm), exsolution of a trigonal phase, with structure analogous to that of Cs<sub>3</sub>H(SeO<sub>4</sub>)<sub>2</sub>, was found to accompany the transformation to the cubic phase. While the driver for this transformation is not fully known, the cell volumes of both the exsolved and matrix phases indicate they are chemically distinct, respectively, from Cs<sub>3</sub>H(SeO<sub>4</sub>)<sub>2</sub> and Cs<sub>2</sub>(HSeO<sub>4</sub>)(H<sub>2</sub>PO<sub>4</sub>), suggesting additional chemical levers for control of transformation behavior.</p></div>","PeriodicalId":431,"journal":{"name":"Solid State Ionics","volume":"416 ","pages":"Article 116690"},"PeriodicalIF":3.0000,"publicationDate":"2024-09-05","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"High temperature phase transformations and Superprotonic conductivity in Cs2(HSeO4)(H2PO4)\",\"authors\":\"Grace Xiong , Ara Jo , Louis S. Wang , Sossina M. Haile\",\"doi\":\"10.1016/j.ssi.2024.116690\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><p>The compound Cs<sub>2</sub>(HSeO<sub>4</sub>)(H<sub>2</sub>PO<sub>4</sub>) is of interest due to its high conductivity in its superprotonic state. In the present work, in situ X-ray diffraction studies, simultaneous thermal analysis, and AC impedance spectroscopy, each performed under controlled value of steam partial pressure (<em>p</em>H<sub>2</sub>O), were carried out to elucidate the crystallographic features of the transformation and resolve the conductivity in the high temperature phase. The studies reveal that the material transforms to a cubic phase at a temperature of approximately 116 °C, that the activation energy for proton transport in the cubic phase is 0.304(2) eV, and the magnitude of the conductivity is comparable to that of Cs<sub>2</sub>(HSO<sub>4</sub>)(H<sub>2</sub>PO<sub>4</sub>). Despite differences in the room temperature structures of Cs<sub>2</sub>(HSeO<sub>4</sub>)(H<sub>2</sub>PO<sub>4</sub>), Cs<sub>2</sub>(HSO<sub>4</sub>)(H<sub>2</sub>PO<sub>4</sub>), and CsH<sub>2</sub>PO<sub>4</sub>, each has a monoclinic to cubic transformation entropy of approximately 23 J/mol(CsH<sub>x</sub>XO<sub>4</sub>)/K. Under <em>p</em>H<sub>2</sub>O = 0.05 atm, the cubic phase of Cs<sub>2</sub>(HSeO<sub>4</sub>)(H<sub>2</sub>PO<sub>4</sub>) is stable to approximately 250 °C. Under elevated <em>p</em>H<sub>2</sub>O (0.3 atm), exsolution of a trigonal phase, with structure analogous to that of Cs<sub>3</sub>H(SeO<sub>4</sub>)<sub>2</sub>, was found to accompany the transformation to the cubic phase. While the driver for this transformation is not fully known, the cell volumes of both the exsolved and matrix phases indicate they are chemically distinct, respectively, from Cs<sub>3</sub>H(SeO<sub>4</sub>)<sub>2</sub> and Cs<sub>2</sub>(HSeO<sub>4</sub>)(H<sub>2</sub>PO<sub>4</sub>), suggesting additional chemical levers for control of transformation behavior.</p></div>\",\"PeriodicalId\":431,\"journal\":{\"name\":\"Solid State Ionics\",\"volume\":\"416 \",\"pages\":\"Article 116690\"},\"PeriodicalIF\":3.0000,\"publicationDate\":\"2024-09-05\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Solid State Ionics\",\"FirstCategoryId\":\"88\",\"ListUrlMain\":\"https://www.sciencedirect.com/science/article/pii/S0167273824002388\",\"RegionNum\":4,\"RegionCategory\":\"材料科学\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q3\",\"JCRName\":\"CHEMISTRY, PHYSICAL\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Solid State Ionics","FirstCategoryId":"88","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S0167273824002388","RegionNum":4,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q3","JCRName":"CHEMISTRY, PHYSICAL","Score":null,"Total":0}
High temperature phase transformations and Superprotonic conductivity in Cs2(HSeO4)(H2PO4)
The compound Cs2(HSeO4)(H2PO4) is of interest due to its high conductivity in its superprotonic state. In the present work, in situ X-ray diffraction studies, simultaneous thermal analysis, and AC impedance spectroscopy, each performed under controlled value of steam partial pressure (pH2O), were carried out to elucidate the crystallographic features of the transformation and resolve the conductivity in the high temperature phase. The studies reveal that the material transforms to a cubic phase at a temperature of approximately 116 °C, that the activation energy for proton transport in the cubic phase is 0.304(2) eV, and the magnitude of the conductivity is comparable to that of Cs2(HSO4)(H2PO4). Despite differences in the room temperature structures of Cs2(HSeO4)(H2PO4), Cs2(HSO4)(H2PO4), and CsH2PO4, each has a monoclinic to cubic transformation entropy of approximately 23 J/mol(CsHxXO4)/K. Under pH2O = 0.05 atm, the cubic phase of Cs2(HSeO4)(H2PO4) is stable to approximately 250 °C. Under elevated pH2O (0.3 atm), exsolution of a trigonal phase, with structure analogous to that of Cs3H(SeO4)2, was found to accompany the transformation to the cubic phase. While the driver for this transformation is not fully known, the cell volumes of both the exsolved and matrix phases indicate they are chemically distinct, respectively, from Cs3H(SeO4)2 and Cs2(HSeO4)(H2PO4), suggesting additional chemical levers for control of transformation behavior.
期刊介绍:
This interdisciplinary journal is devoted to the physics, chemistry and materials science of diffusion, mass transport, and reactivity of solids. The major part of each issue is devoted to articles on:
(i) physics and chemistry of defects in solids;
(ii) reactions in and on solids, e.g. intercalation, corrosion, oxidation, sintering;
(iii) ion transport measurements, mechanisms and theory;
(iv) solid state electrochemistry;
(v) ionically-electronically mixed conducting solids.
Related technological applications are also included, provided their characteristics are interpreted in terms of the basic solid state properties.
Review papers and relevant symposium proceedings are welcome.