{"title":"机械损耗光谱法研究立方氧化锆缺陷","authors":"M. Weller, A. Lakki","doi":"10.1002/bbpc.199700042","DOIUrl":null,"url":null,"abstract":"<p>In cubic Y<sub>2</sub>O<sub>3</sub> (10–25 mol%) or CaO (14 and 17 mol%) stabilized ZrO<sub>2</sub>, oxygen vacancies are created as charge-compensating defects. Mechanical loss (internal friction) measurements are performed on single crystals of cubic zirconia with various orientation at frequencies of <i>f</i> ≈︁ 1 Hz and 1 kHz, to study the local crystallographic structure of the defects. The mechanical spectra show a composite loss maximum at 400–600 K consisting of two overlapping submaxima: I and I<sub>A</sub> in ZrO<sub>2</sub>-Y<sub>2</sub>O<sub>3</sub>; I' and I'<sub>A</sub> in ZrO<sub>2</sub>-CaO. Submaxima I (I') are assigned to defect pairs of oxygen vacancies and impurity atoms forming elastic (and electric) dipoles. These are oriented parallel to <111>, with the vacancy on nearest neighbour sites (trigonal symmetry). Submaxima I<sub>A</sub>(I'<sub>A</sub>) are attributed to relaxation of vacancies within Y- (or Ca-) clusters with various sizes and configurations corresponding to lower defect symmetry. The electrical conductivity (4 probe d.c. technique) decreases for concentrations ≥10mol% Y<sub>2</sub>O<sub>3</sub>, whereas the activation enthalpy increases with Y<sub>2</sub>O<sub>3</sub> content. A high temperature peak C in ZrO<sub>2</sub>-CaO around 1400 K (0.1 Hz) is probably due to local atomic jumps of cations.</p>","PeriodicalId":100156,"journal":{"name":"Berichte der Bunsengesellschaft für physikalische Chemie","volume":"101 9","pages":"1297-1303"},"PeriodicalIF":0.0000,"publicationDate":"2014-03-18","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1002/bbpc.199700042","citationCount":"12","resultStr":"{\"title\":\"Defects in Cubic Zirconia Studied by Mechanical Loss Spectroscopy\",\"authors\":\"M. Weller, A. Lakki\",\"doi\":\"10.1002/bbpc.199700042\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<p>In cubic Y<sub>2</sub>O<sub>3</sub> (10–25 mol%) or CaO (14 and 17 mol%) stabilized ZrO<sub>2</sub>, oxygen vacancies are created as charge-compensating defects. Mechanical loss (internal friction) measurements are performed on single crystals of cubic zirconia with various orientation at frequencies of <i>f</i> ≈︁ 1 Hz and 1 kHz, to study the local crystallographic structure of the defects. The mechanical spectra show a composite loss maximum at 400–600 K consisting of two overlapping submaxima: I and I<sub>A</sub> in ZrO<sub>2</sub>-Y<sub>2</sub>O<sub>3</sub>; I' and I'<sub>A</sub> in ZrO<sub>2</sub>-CaO. Submaxima I (I') are assigned to defect pairs of oxygen vacancies and impurity atoms forming elastic (and electric) dipoles. These are oriented parallel to <111>, with the vacancy on nearest neighbour sites (trigonal symmetry). Submaxima I<sub>A</sub>(I'<sub>A</sub>) are attributed to relaxation of vacancies within Y- (or Ca-) clusters with various sizes and configurations corresponding to lower defect symmetry. The electrical conductivity (4 probe d.c. technique) decreases for concentrations ≥10mol% Y<sub>2</sub>O<sub>3</sub>, whereas the activation enthalpy increases with Y<sub>2</sub>O<sub>3</sub> content. A high temperature peak C in ZrO<sub>2</sub>-CaO around 1400 K (0.1 Hz) is probably due to local atomic jumps of cations.</p>\",\"PeriodicalId\":100156,\"journal\":{\"name\":\"Berichte der Bunsengesellschaft für physikalische Chemie\",\"volume\":\"101 9\",\"pages\":\"1297-1303\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2014-03-18\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"https://sci-hub-pdf.com/10.1002/bbpc.199700042\",\"citationCount\":\"12\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Berichte der Bunsengesellschaft für physikalische Chemie\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://onlinelibrary.wiley.com/doi/10.1002/bbpc.199700042\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Berichte der Bunsengesellschaft für physikalische Chemie","FirstCategoryId":"1085","ListUrlMain":"https://onlinelibrary.wiley.com/doi/10.1002/bbpc.199700042","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Defects in Cubic Zirconia Studied by Mechanical Loss Spectroscopy
In cubic Y2O3 (10–25 mol%) or CaO (14 and 17 mol%) stabilized ZrO2, oxygen vacancies are created as charge-compensating defects. Mechanical loss (internal friction) measurements are performed on single crystals of cubic zirconia with various orientation at frequencies of f ≈︁ 1 Hz and 1 kHz, to study the local crystallographic structure of the defects. The mechanical spectra show a composite loss maximum at 400–600 K consisting of two overlapping submaxima: I and IA in ZrO2-Y2O3; I' and I'A in ZrO2-CaO. Submaxima I (I') are assigned to defect pairs of oxygen vacancies and impurity atoms forming elastic (and electric) dipoles. These are oriented parallel to <111>, with the vacancy on nearest neighbour sites (trigonal symmetry). Submaxima IA(I'A) are attributed to relaxation of vacancies within Y- (or Ca-) clusters with various sizes and configurations corresponding to lower defect symmetry. The electrical conductivity (4 probe d.c. technique) decreases for concentrations ≥10mol% Y2O3, whereas the activation enthalpy increases with Y2O3 content. A high temperature peak C in ZrO2-CaO around 1400 K (0.1 Hz) is probably due to local atomic jumps of cations.