K. Mehta, Yuh-Shiuan Liu, Jialin Wang, Hoon Jeong, T. Detchprohm, Young Jae Park, S. Shen, R. Dupuis, P. Yoder
{"title":"Theory and Design of Electron Blocking Layers for III-N Based Laser Diodes by Numerical Simulation","authors":"K. Mehta, Yuh-Shiuan Liu, Jialin Wang, Hoon Jeong, T. Detchprohm, Young Jae Park, S. Shen, R. Dupuis, P. Yoder","doi":"10.1109/DRC.2018.8442243","DOIUrl":null,"url":null,"abstract":"Unlike laser diodes made of traditional III-V materials (III-AsP), III-Nitride laser diodes and LEDs suffer from reduced injection efficiency due to greater electron leakage [1]. The overflow of electrons out of the active region into the adjacent p-type quasi-neutral region (QNR) is primarily due to the asymmetry between majority carrier conductivities in p- and n-GaN [2], where the electron conductivity in n-GaN is more than 40 times greater than the hole conductivity in p-GaN [3], [4]. Furthermore, carrier leakage is exacerbated by interfacial spontaneous and piezoelectric polarization charges at III-N heterojunctions. To stem electron leakage, an electron blocking layer (EBL) is typically employed between the last quantum barrier (QB) and p-type quasi-neutral region (QNR), and this EBL is typically a thin layer of wide bandgap material.","PeriodicalId":269641,"journal":{"name":"2018 76th Device Research Conference (DRC)","volume":"3 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2018-06-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"10","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"2018 76th Device Research Conference (DRC)","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/DRC.2018.8442243","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 10
Abstract
Unlike laser diodes made of traditional III-V materials (III-AsP), III-Nitride laser diodes and LEDs suffer from reduced injection efficiency due to greater electron leakage [1]. The overflow of electrons out of the active region into the adjacent p-type quasi-neutral region (QNR) is primarily due to the asymmetry between majority carrier conductivities in p- and n-GaN [2], where the electron conductivity in n-GaN is more than 40 times greater than the hole conductivity in p-GaN [3], [4]. Furthermore, carrier leakage is exacerbated by interfacial spontaneous and piezoelectric polarization charges at III-N heterojunctions. To stem electron leakage, an electron blocking layer (EBL) is typically employed between the last quantum barrier (QB) and p-type quasi-neutral region (QNR), and this EBL is typically a thin layer of wide bandgap material.