Tim H. Reuter, Lkhamsuren Bayarjargal, Daniel Rytz, Sebastian Schwung, Victor Milman, Björn Winkler
{"title":"Pressure- and Temperature-Dependence of Polar Nanoregions in KTN40 (KTa0.6Nb0.4O3) and KNbO3","authors":"Tim H. Reuter, Lkhamsuren Bayarjargal, Daniel Rytz, Sebastian Schwung, Victor Milman, Björn Winkler","doi":"10.1021/acs.jpcc.5c01075","DOIUrl":null,"url":null,"abstract":"We investigated the pressure- and temperature-dependent phase transitions in KTN<sub>40</sub> (KTa<sub>0.6</sub>Nb<sub>0.4</sub>O<sub>3</sub>) and KNbO<sub>3</sub>, two members of the perovskite-type ferroelectric solid solution system KTN (KTa<sub><i>x</i></sub>Nb<sub>1–<i>x</i></sub>O<sub>3</sub>), by heat capacity measurements, Raman spectroscopy, and second harmonic generation (SHG). The phase transition temperatures for the rhombohedral → orthorhombic → tetragonal → cubic sequence in KTN<sub>40</sub> were determined to be 180(2) K, 225(2) K, and 295(2) K, respectively, by heat capacity measurements. For KNbO<sub>3</sub>, SHG measurements revealed orthorhombic → tetragonal → cubic transitions at 460(3) K and 720(3) K. In both compounds, SHG experiments indicated the presence of polar nanoregions within the cubic phase above the Curie temperatures of KTN<sub>40</sub> and KNbO<sub>3</sub>. The dynamics and stability fields of these polar nanoregions were analyzed, resulting in Burns temperatures <i>T</i><sub>d</sub> of 510(5) K for KTN<sub>40</sub> and 1000(5) K for KNbO<sub>3</sub>. Intermediate temperatures, <i>T</i>*, where polar nanoregions begin to merge into larger domains, were identified for KTN<sub>40</sub> and KNbO<sub>3</sub> to be 350(5) K and 775(5) K, respectively. The pressure-dependent tetragonal → cubic phase transition was observed at 1.3(1) GPa for KTN<sub>40</sub> and 15(0.5) GPa for KNbO<sub>3</sub> using SHG. SHG measurements further confirmed polar nanoregions occurring in the cubic phase above the Curie pressures of KTN<sub>40</sub> and KNbO<sub>3</sub>. Burns pressures <i>p</i><sub>d</sub> were determined to be 6(1) GPa for KTN<sub>40</sub> and 24(1) GPa and intermediate pressures <i>p</i>* were found at 1.8(2) GPa and 17(1) GPa, respectively. The known phase boundaries in temperature- and pressure-dependent phase diagrams could be reproduced and extended and phase diagrams could be enhanced by the addition of stability fields of polar nanoregions. It could also be shown that the dynamics of the polar nanoregions depend on chemical composition, as temperature-induced polar nanoregions in KTN<sub>40</sub> appear to be smaller than in KNbO<sub>3</sub>. In addition, this study contains thermodynamic data for KNbO<sub>3</sub>, KTN<sub>40</sub> and KTaO<sub>3</sub>. Based on the excess entropy for KTN<sub>40</sub>, these show that the formation of solid solutions tends to be favored in the KTN system compared to segregation.","PeriodicalId":61,"journal":{"name":"The Journal of Physical Chemistry C","volume":"23 1","pages":""},"PeriodicalIF":3.3000,"publicationDate":"2025-04-24","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"The Journal of Physical Chemistry C","FirstCategoryId":"1","ListUrlMain":"https://doi.org/10.1021/acs.jpcc.5c01075","RegionNum":3,"RegionCategory":"化学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"CHEMISTRY, PHYSICAL","Score":null,"Total":0}
引用次数: 0
Abstract
We investigated the pressure- and temperature-dependent phase transitions in KTN40 (KTa0.6Nb0.4O3) and KNbO3, two members of the perovskite-type ferroelectric solid solution system KTN (KTaxNb1–xO3), by heat capacity measurements, Raman spectroscopy, and second harmonic generation (SHG). The phase transition temperatures for the rhombohedral → orthorhombic → tetragonal → cubic sequence in KTN40 were determined to be 180(2) K, 225(2) K, and 295(2) K, respectively, by heat capacity measurements. For KNbO3, SHG measurements revealed orthorhombic → tetragonal → cubic transitions at 460(3) K and 720(3) K. In both compounds, SHG experiments indicated the presence of polar nanoregions within the cubic phase above the Curie temperatures of KTN40 and KNbO3. The dynamics and stability fields of these polar nanoregions were analyzed, resulting in Burns temperatures Td of 510(5) K for KTN40 and 1000(5) K for KNbO3. Intermediate temperatures, T*, where polar nanoregions begin to merge into larger domains, were identified for KTN40 and KNbO3 to be 350(5) K and 775(5) K, respectively. The pressure-dependent tetragonal → cubic phase transition was observed at 1.3(1) GPa for KTN40 and 15(0.5) GPa for KNbO3 using SHG. SHG measurements further confirmed polar nanoregions occurring in the cubic phase above the Curie pressures of KTN40 and KNbO3. Burns pressures pd were determined to be 6(1) GPa for KTN40 and 24(1) GPa and intermediate pressures p* were found at 1.8(2) GPa and 17(1) GPa, respectively. The known phase boundaries in temperature- and pressure-dependent phase diagrams could be reproduced and extended and phase diagrams could be enhanced by the addition of stability fields of polar nanoregions. It could also be shown that the dynamics of the polar nanoregions depend on chemical composition, as temperature-induced polar nanoregions in KTN40 appear to be smaller than in KNbO3. In addition, this study contains thermodynamic data for KNbO3, KTN40 and KTaO3. Based on the excess entropy for KTN40, these show that the formation of solid solutions tends to be favored in the KTN system compared to segregation.
期刊介绍:
The Journal of Physical Chemistry A/B/C is devoted to reporting new and original experimental and theoretical basic research of interest to physical chemists, biophysical chemists, and chemical physicists.