{"title":"Simulation of Hot-Electron Effects with Multi-band Semiconductor Devices","authors":"L. P. Tatum, Madeline Sciullo, M. Law","doi":"10.1109/SISPAD.2018.8551626","DOIUrl":null,"url":null,"abstract":"In this work, we present a 2-Valley energy band model of electron transport that delivers more accurate solutions compared with the Farahmand model but with improved convergence and a faster solution time for very high electric fields. This was achieved by implementing the Fermi-Dirac integral distribution as a substitution for the Boltzmann exponential, electron carrier temperature due to heat generation and conduction in the semiconductor lattice, and additional electron concentration modeling for a second conduction energy band minima. The model was primarily tuned by varying the electron temperature relaxation time constant. It was tested using a GaN-based High Electron Mobility Transistor using the Finite-Element Quasi Fermi method.","PeriodicalId":170070,"journal":{"name":"2018 International Conference on Simulation of Semiconductor Processes and Devices (SISPAD)","volume":"128 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2018-09-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"3","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"2018 International Conference on Simulation of Semiconductor Processes and Devices (SISPAD)","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/SISPAD.2018.8551626","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 3
Abstract
In this work, we present a 2-Valley energy band model of electron transport that delivers more accurate solutions compared with the Farahmand model but with improved convergence and a faster solution time for very high electric fields. This was achieved by implementing the Fermi-Dirac integral distribution as a substitution for the Boltzmann exponential, electron carrier temperature due to heat generation and conduction in the semiconductor lattice, and additional electron concentration modeling for a second conduction energy band minima. The model was primarily tuned by varying the electron temperature relaxation time constant. It was tested using a GaN-based High Electron Mobility Transistor using the Finite-Element Quasi Fermi method.