{"title":"金属氧化物半导体(MOS)结构的表面电荷密度研究延伸到金属铁电金属(MFM)结构的本体极化研究:极化数据的实验与模拟","authors":"Syed Mahboob, None Rizwana","doi":"10.1080/10584587.2023.2239096","DOIUrl":null,"url":null,"abstract":"Ba(NdxTi(1-2x)Nbx)O3 and (Na0.5Bi0.5)(NdyTi1-2yNby)O3 relaxor ferroelectric materials were prepared through solid state sintering route. The polarization as a function of electric field (PE loops) were measured with Radiant technologies PE loop tracer. In the present studies we have extended the surface charge density studies of metal oxide semiconductor (MOS) structure to the polarization studies of metal ferroelectric and metal (MFM) structure in bulk form by combining it with the modified Glazounov and Arrhenius equations. The simulation is in good agreement the experimental data. In the case of Ba(NdxTi(1-2x)Nbx)O3 ceramics the value of dipole moment (p) are 2.24x10−26 C.m, 1.80x10−26 C.m, 2.23x10−26 C.m & 2.21x 10−26 C.m for x = 0.025, 0.05, 0.1 & 0.2, respectively. The values of surface potential (Ψp) are 466 meV, 503 meV, 552 meV & 505 meV for x = 0.025, 0.05, 0.1 & 0.2, respectively.","PeriodicalId":13686,"journal":{"name":"Integrated Ferroelectrics","volume":"17 1","pages":"0"},"PeriodicalIF":0.7000,"publicationDate":"2023-09-02","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Extension of Surface Charge Density Studies of Metal Oxide Semiconductor (MOS) Structure to Polarization Studies of Metal Ferroelectric Metal (MFM) Structure in Bulk Form: Experimental and Simulation of Polarization Data\",\"authors\":\"Syed Mahboob, None Rizwana\",\"doi\":\"10.1080/10584587.2023.2239096\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Ba(NdxTi(1-2x)Nbx)O3 and (Na0.5Bi0.5)(NdyTi1-2yNby)O3 relaxor ferroelectric materials were prepared through solid state sintering route. The polarization as a function of electric field (PE loops) were measured with Radiant technologies PE loop tracer. In the present studies we have extended the surface charge density studies of metal oxide semiconductor (MOS) structure to the polarization studies of metal ferroelectric and metal (MFM) structure in bulk form by combining it with the modified Glazounov and Arrhenius equations. The simulation is in good agreement the experimental data. In the case of Ba(NdxTi(1-2x)Nbx)O3 ceramics the value of dipole moment (p) are 2.24x10−26 C.m, 1.80x10−26 C.m, 2.23x10−26 C.m & 2.21x 10−26 C.m for x = 0.025, 0.05, 0.1 & 0.2, respectively. The values of surface potential (Ψp) are 466 meV, 503 meV, 552 meV & 505 meV for x = 0.025, 0.05, 0.1 & 0.2, respectively.\",\"PeriodicalId\":13686,\"journal\":{\"name\":\"Integrated Ferroelectrics\",\"volume\":\"17 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.7000,\"publicationDate\":\"2023-09-02\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Integrated Ferroelectrics\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1080/10584587.2023.2239096\",\"RegionNum\":4,\"RegionCategory\":\"工程技术\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q4\",\"JCRName\":\"ENGINEERING, ELECTRICAL & ELECTRONIC\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Integrated Ferroelectrics","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1080/10584587.2023.2239096","RegionNum":4,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q4","JCRName":"ENGINEERING, ELECTRICAL & ELECTRONIC","Score":null,"Total":0}
Extension of Surface Charge Density Studies of Metal Oxide Semiconductor (MOS) Structure to Polarization Studies of Metal Ferroelectric Metal (MFM) Structure in Bulk Form: Experimental and Simulation of Polarization Data
Ba(NdxTi(1-2x)Nbx)O3 and (Na0.5Bi0.5)(NdyTi1-2yNby)O3 relaxor ferroelectric materials were prepared through solid state sintering route. The polarization as a function of electric field (PE loops) were measured with Radiant technologies PE loop tracer. In the present studies we have extended the surface charge density studies of metal oxide semiconductor (MOS) structure to the polarization studies of metal ferroelectric and metal (MFM) structure in bulk form by combining it with the modified Glazounov and Arrhenius equations. The simulation is in good agreement the experimental data. In the case of Ba(NdxTi(1-2x)Nbx)O3 ceramics the value of dipole moment (p) are 2.24x10−26 C.m, 1.80x10−26 C.m, 2.23x10−26 C.m & 2.21x 10−26 C.m for x = 0.025, 0.05, 0.1 & 0.2, respectively. The values of surface potential (Ψp) are 466 meV, 503 meV, 552 meV & 505 meV for x = 0.025, 0.05, 0.1 & 0.2, respectively.
期刊介绍:
Integrated Ferroelectrics provides an international, interdisciplinary forum for electronic engineers and physicists as well as process and systems engineers, ceramicists, and chemists who are involved in research, design, development, manufacturing and utilization of integrated ferroelectric devices. Such devices unite ferroelectric films and semiconductor integrated circuit chips. The result is a new family of electronic devices, which combine the unique nonvolatile memory, pyroelectric, piezoelectric, photorefractive, radiation-hard, acoustic and/or dielectric properties of ferroelectric materials with the dynamic memory, logic and/or amplification properties and miniaturization and low-cost advantages of semiconductor i.c. technology.