{"title":"带AlN缓冲液的AlGaN通道hemt的极化和击穿分析","authors":"Godwin Raj, Mohan Kumar, C. Sarkar","doi":"10.4236/WJCMP.2015.53024","DOIUrl":null,"url":null,"abstract":"We have demonstrated the first carrier density model for AlGaN channel with AlN buffer using spontaneous and piezoelectric polarization comparison with experimental and theoretical results. From the results we proved that the formation of 2DEG in undoped structure relied both on spontaneous and piezoelectric polarization. The electron distribution of Al concentration (0 < x < 0.5) was measured for both AlGaN channel and barrier. Barrier thickness assumed between 20 and 25 nm for validating the experimental results. The carrier concentration was observed at the specific interface of the N- and Ga-face by assuming x1, x2 = 0. The model results are verified with previously reported experimental data.","PeriodicalId":308307,"journal":{"name":"World Journal of Condensed Matter Physics","volume":"31 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2015-07-27","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"1","resultStr":"{\"title\":\"Polarization and Breakdown Analysis of AlGaN Channel HEMTs with AlN Buffer\",\"authors\":\"Godwin Raj, Mohan Kumar, C. Sarkar\",\"doi\":\"10.4236/WJCMP.2015.53024\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"We have demonstrated the first carrier density model for AlGaN channel with AlN buffer using spontaneous and piezoelectric polarization comparison with experimental and theoretical results. From the results we proved that the formation of 2DEG in undoped structure relied both on spontaneous and piezoelectric polarization. The electron distribution of Al concentration (0 < x < 0.5) was measured for both AlGaN channel and barrier. Barrier thickness assumed between 20 and 25 nm for validating the experimental results. The carrier concentration was observed at the specific interface of the N- and Ga-face by assuming x1, x2 = 0. The model results are verified with previously reported experimental data.\",\"PeriodicalId\":308307,\"journal\":{\"name\":\"World Journal of Condensed Matter Physics\",\"volume\":\"31 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2015-07-27\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"1\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"World Journal of Condensed Matter Physics\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.4236/WJCMP.2015.53024\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"World Journal of Condensed Matter Physics","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.4236/WJCMP.2015.53024","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 1
摘要
我们利用自发极化和压电极化与实验和理论结果进行了比较,证明了具有AlN缓冲的AlGaN通道的第一个载流子密度模型。结果表明,在非掺杂结构中,2DEG的形成既依赖于自发极化,也依赖于压电极化。测量了AlGaN通道和势垒中Al浓度(0 < x < 0.5)的电子分布。为了验证实验结果,假设障壁厚度在20 ~ 25nm之间。假设x1, x2 = 0,观察N面和ga面特定界面的载流子浓度。模型结果与先前报道的实验数据进行了验证。
Polarization and Breakdown Analysis of AlGaN Channel HEMTs with AlN Buffer
We have demonstrated the first carrier density model for AlGaN channel with AlN buffer using spontaneous and piezoelectric polarization comparison with experimental and theoretical results. From the results we proved that the formation of 2DEG in undoped structure relied both on spontaneous and piezoelectric polarization. The electron distribution of Al concentration (0 < x < 0.5) was measured for both AlGaN channel and barrier. Barrier thickness assumed between 20 and 25 nm for validating the experimental results. The carrier concentration was observed at the specific interface of the N- and Ga-face by assuming x1, x2 = 0. The model results are verified with previously reported experimental data.