{"title":"镧掺杂SrBi4Ti4O15铁电陶瓷的介电性能和铁电性能","authors":"K. Ashok, V. Raju, S. Chandralingam, P. Sarah","doi":"10.1109/IVEC.2011.5747039","DOIUrl":null,"url":null,"abstract":"Bismuth layer structure ferroelectrics (BLSFs) have attracted intensive investigation for the potential use in non volatile ferroelectric random access memory (FeRAM) and piezoelectric devices suitable at high temperature. Bismuth layere structured compounds with general formula of (Bi<inf>2</inf>O<inf>2</inf>)<sup>2+</sup> (A<inf>m−1</inf>B<inf>m</inf>O<inf>3m+1</inf>)<sup>2−</sup> are firstly found by Aurivillius<sup>1–3</sup>. The structure of these compounds can be described as pseudo-pervoskite (A<inf>m−1</inf>B<inf>m</inf>O<inf>3m+1</inf>)<sup>2−</sup> slabs separated by (Bi<inf>2</inf>O<inf>2</inf>)<sup>2+</sup> layeres along the crystallographic c-axis<sup>4</sup>. The 12-coordinated A site can be occupied by such cations as La<sup>3+</sup>, Bi<sup>3+</sup>, Ba<sup>2+</sup>, Sr<sup>2+</sup>, Pb<sup>2+</sup>, Ca<sup>2+</sup>, Na<sup>+</sup>, etc. While the octahedral-coordinated B site can be occupied by W<sup>6+</sup>, Nb<sup>5+</sup>, Ta<sup>5+</sup>, Ti<sup>4+</sup>, etc. Lanthanum substituted BiT (Bi<inf>4</inf>Ti<inf>4</inf>O<inf>12</inf>) known as BLT has been extensively investigated. With this substitution, BLT shows relatively large P<inf>r</inf>, low synthesis temperature and good fatigue endurance which makes it a potential candidate for FeRAM application. So, lanthanum doping is an effective way to improve the ferroelectric and fatigue properties of Bi<inf>4</inf>Ti<inf>4</inf>O<inf>12</inf>. Lanthanum doped Bismuth layer structure ferroelectrics (BLSFs) ceramics SrBi<inf>4−x</inf>La <inf>x</inf>Ti<inf>4</inf>O<inf>15</inf> (x=0, 0.025, 0.050, 0.075, 0.1) were prepared by solid state reaction method. X-Ray diffraction pattern showed that single phase was formed when x=0− 0.1. Morphological studies were carried out by SEM analysis. It was found that crystal lattice constant, dielectric and electrical properties of SBT ferroelectrics varied appreciably with amount of doping. Dielectric measurements in the frequency range 100Hz–1MHz were made using an impedance analyzer (Wayne Kerr 6500P) and the measurements were carried out from RT to 600°C. The ferroelectric hysteresis loop was traced at room temperature by a standard P-E loop tracer based on sawyer-tower circuit. The values of 2P<inf>r</inf> and E<inf>c</inf> for pure and lanthanum doped SBT are given in the following table.","PeriodicalId":106174,"journal":{"name":"2011 IEEE International Vacuum Electronics Conference (IVEC)","volume":"27 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2011-02-21","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Dielectric and ferroelectric properties of lanthanum doped SrBi4Ti4O15 ferroelectric ceramics\",\"authors\":\"K. Ashok, V. Raju, S. Chandralingam, P. Sarah\",\"doi\":\"10.1109/IVEC.2011.5747039\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Bismuth layer structure ferroelectrics (BLSFs) have attracted intensive investigation for the potential use in non volatile ferroelectric random access memory (FeRAM) and piezoelectric devices suitable at high temperature. Bismuth layere structured compounds with general formula of (Bi<inf>2</inf>O<inf>2</inf>)<sup>2+</sup> (A<inf>m−1</inf>B<inf>m</inf>O<inf>3m+1</inf>)<sup>2−</sup> are firstly found by Aurivillius<sup>1–3</sup>. The structure of these compounds can be described as pseudo-pervoskite (A<inf>m−1</inf>B<inf>m</inf>O<inf>3m+1</inf>)<sup>2−</sup> slabs separated by (Bi<inf>2</inf>O<inf>2</inf>)<sup>2+</sup> layeres along the crystallographic c-axis<sup>4</sup>. The 12-coordinated A site can be occupied by such cations as La<sup>3+</sup>, Bi<sup>3+</sup>, Ba<sup>2+</sup>, Sr<sup>2+</sup>, Pb<sup>2+</sup>, Ca<sup>2+</sup>, Na<sup>+</sup>, etc. While the octahedral-coordinated B site can be occupied by W<sup>6+</sup>, Nb<sup>5+</sup>, Ta<sup>5+</sup>, Ti<sup>4+</sup>, etc. Lanthanum substituted BiT (Bi<inf>4</inf>Ti<inf>4</inf>O<inf>12</inf>) known as BLT has been extensively investigated. With this substitution, BLT shows relatively large P<inf>r</inf>, low synthesis temperature and good fatigue endurance which makes it a potential candidate for FeRAM application. So, lanthanum doping is an effective way to improve the ferroelectric and fatigue properties of Bi<inf>4</inf>Ti<inf>4</inf>O<inf>12</inf>. Lanthanum doped Bismuth layer structure ferroelectrics (BLSFs) ceramics SrBi<inf>4−x</inf>La <inf>x</inf>Ti<inf>4</inf>O<inf>15</inf> (x=0, 0.025, 0.050, 0.075, 0.1) were prepared by solid state reaction method. X-Ray diffraction pattern showed that single phase was formed when x=0− 0.1. Morphological studies were carried out by SEM analysis. It was found that crystal lattice constant, dielectric and electrical properties of SBT ferroelectrics varied appreciably with amount of doping. Dielectric measurements in the frequency range 100Hz–1MHz were made using an impedance analyzer (Wayne Kerr 6500P) and the measurements were carried out from RT to 600°C. The ferroelectric hysteresis loop was traced at room temperature by a standard P-E loop tracer based on sawyer-tower circuit. The values of 2P<inf>r</inf> and E<inf>c</inf> for pure and lanthanum doped SBT are given in the following table.\",\"PeriodicalId\":106174,\"journal\":{\"name\":\"2011 IEEE International Vacuum Electronics Conference (IVEC)\",\"volume\":\"27 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2011-02-21\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"2011 IEEE International Vacuum Electronics Conference (IVEC)\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/IVEC.2011.5747039\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"2011 IEEE International Vacuum Electronics Conference (IVEC)","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/IVEC.2011.5747039","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Dielectric and ferroelectric properties of lanthanum doped SrBi4Ti4O15 ferroelectric ceramics
Bismuth layer structure ferroelectrics (BLSFs) have attracted intensive investigation for the potential use in non volatile ferroelectric random access memory (FeRAM) and piezoelectric devices suitable at high temperature. Bismuth layere structured compounds with general formula of (Bi2O2)2+ (Am−1BmO3m+1)2− are firstly found by Aurivillius1–3. The structure of these compounds can be described as pseudo-pervoskite (Am−1BmO3m+1)2− slabs separated by (Bi2O2)2+ layeres along the crystallographic c-axis4. The 12-coordinated A site can be occupied by such cations as La3+, Bi3+, Ba2+, Sr2+, Pb2+, Ca2+, Na+, etc. While the octahedral-coordinated B site can be occupied by W6+, Nb5+, Ta5+, Ti4+, etc. Lanthanum substituted BiT (Bi4Ti4O12) known as BLT has been extensively investigated. With this substitution, BLT shows relatively large Pr, low synthesis temperature and good fatigue endurance which makes it a potential candidate for FeRAM application. So, lanthanum doping is an effective way to improve the ferroelectric and fatigue properties of Bi4Ti4O12. Lanthanum doped Bismuth layer structure ferroelectrics (BLSFs) ceramics SrBi4−xLa xTi4O15 (x=0, 0.025, 0.050, 0.075, 0.1) were prepared by solid state reaction method. X-Ray diffraction pattern showed that single phase was formed when x=0− 0.1. Morphological studies were carried out by SEM analysis. It was found that crystal lattice constant, dielectric and electrical properties of SBT ferroelectrics varied appreciably with amount of doping. Dielectric measurements in the frequency range 100Hz–1MHz were made using an impedance analyzer (Wayne Kerr 6500P) and the measurements were carried out from RT to 600°C. The ferroelectric hysteresis loop was traced at room temperature by a standard P-E loop tracer based on sawyer-tower circuit. The values of 2Pr and Ec for pure and lanthanum doped SBT are given in the following table.