Y. Wimmer, S. Tyaginov, F. Rudolf, K. Rupp, M. Bina, H. Enichlmair, J.M. Park, R. Minixhofer, H. Ceric, T. Grasser
{"title":"nLDMOS晶体管热载流子退化的物理建模","authors":"Y. Wimmer, S. Tyaginov, F. Rudolf, K. Rupp, M. Bina, H. Enichlmair, J.M. Park, R. Minixhofer, H. Ceric, T. Grasser","doi":"10.1109/IIRW.2014.7049511","DOIUrl":null,"url":null,"abstract":"Our physics-based HCD model has been validated using scaled CMOS transistors in our previous work. In this work we apply this model for the first time to a high-voltage nLDMOS device. For the calculation of the degrading behaviour the Boltzmann transport equation solver ViennaSHE is used which also requires high quality adaptive meshing. We discuss the influence of the different model components in the different device regions. Finally we compare the model to experimental degradation results and show that each one gives a significant contribution to the result and that all of them are needed in order to satisfactorily fit the experimental data.","PeriodicalId":260079,"journal":{"name":"2014 IEEE International Integrated Reliability Workshop Final Report (IIRW)","volume":"18 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2014-10-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"6","resultStr":"{\"title\":\"Physical modeling of hot-carrier degradation in nLDMOS transistors\",\"authors\":\"Y. Wimmer, S. Tyaginov, F. Rudolf, K. Rupp, M. Bina, H. Enichlmair, J.M. Park, R. Minixhofer, H. Ceric, T. Grasser\",\"doi\":\"10.1109/IIRW.2014.7049511\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Our physics-based HCD model has been validated using scaled CMOS transistors in our previous work. In this work we apply this model for the first time to a high-voltage nLDMOS device. For the calculation of the degrading behaviour the Boltzmann transport equation solver ViennaSHE is used which also requires high quality adaptive meshing. We discuss the influence of the different model components in the different device regions. Finally we compare the model to experimental degradation results and show that each one gives a significant contribution to the result and that all of them are needed in order to satisfactorily fit the experimental data.\",\"PeriodicalId\":260079,\"journal\":{\"name\":\"2014 IEEE International Integrated Reliability Workshop Final Report (IIRW)\",\"volume\":\"18 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2014-10-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"6\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"2014 IEEE International Integrated Reliability Workshop Final Report (IIRW)\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/IIRW.2014.7049511\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"2014 IEEE International Integrated Reliability Workshop Final Report (IIRW)","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/IIRW.2014.7049511","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Physical modeling of hot-carrier degradation in nLDMOS transistors
Our physics-based HCD model has been validated using scaled CMOS transistors in our previous work. In this work we apply this model for the first time to a high-voltage nLDMOS device. For the calculation of the degrading behaviour the Boltzmann transport equation solver ViennaSHE is used which also requires high quality adaptive meshing. We discuss the influence of the different model components in the different device regions. Finally we compare the model to experimental degradation results and show that each one gives a significant contribution to the result and that all of them are needed in order to satisfactorily fit the experimental data.