{"title":"GaN/Inx Ga1-x N/B0.01 Ga0.99 N双异质结场效应晶体管h - fet,用于电子电源应用。","authors":"A. Belarbi, A. Hamdoune","doi":"10.1109/CCSSP49278.2020.9151785","DOIUrl":null,"url":null,"abstract":"This paper aims to study a GaN/In$_{x} Ga_{1}xN/B_{0.01} Ga_{0.99}$ N Double Heterojunction Field Effect Transistor (DH-FET) by using SILVACO TCAD two and three dimensional device simulator. The structure is based on an undoped In$_{x} Ga_{1} x$ N as channel layer and an undopped back-barrier layer of B$_{x} Ga_{1-x}$N. The thickness of the channel layer has been fixed at 10 nm and we change the indium content in the alloy In$_{x} Ga_{1-x}$N of the channel layer, 10%, 25%, 50%, 75%, and 100% to get a channel layer only with nitride indium (InN). Some DC and AC performances of the transistor are simulated for each indium concentration.The increase of indium concentration in the In$_{x} Ga_{1-x}$N channel significantly improves the performances due to its excellent electrical properties and deep quantum well, and the introduction of resistive material B$_{x} Ga_{1-x}$N as back barrier layer with 1% of boron concentration serves to improve the performances due to better confinement of (2DEG) two dimensional electron gas. With 20 nm gate length, the transistor demonstrates a maximum drain-source current (Ids) of 1.2 A/mm, a maximum transconductance (gm) of 425 mS mm$^{-1}$, a gate-leakage current of 3.10$^{-9}$ A, a cut-off frequency (Ft) of 850 GHz, and a maximum oscillation frequency (Fmax) of 1.5 THz.","PeriodicalId":401063,"journal":{"name":"020 1st International Conference on Communications, Control Systems and Signal Processing (CCSSP)","volume":"5 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2020-05-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"GaN/Inx Ga1-x N/B0.01 Ga0.99 N Double Heterojunction Field Effect Transistor DH-FET for electronics power application.\",\"authors\":\"A. Belarbi, A. Hamdoune\",\"doi\":\"10.1109/CCSSP49278.2020.9151785\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"This paper aims to study a GaN/In$_{x} Ga_{1}xN/B_{0.01} Ga_{0.99}$ N Double Heterojunction Field Effect Transistor (DH-FET) by using SILVACO TCAD two and three dimensional device simulator. The structure is based on an undoped In$_{x} Ga_{1} x$ N as channel layer and an undopped back-barrier layer of B$_{x} Ga_{1-x}$N. The thickness of the channel layer has been fixed at 10 nm and we change the indium content in the alloy In$_{x} Ga_{1-x}$N of the channel layer, 10%, 25%, 50%, 75%, and 100% to get a channel layer only with nitride indium (InN). Some DC and AC performances of the transistor are simulated for each indium concentration.The increase of indium concentration in the In$_{x} Ga_{1-x}$N channel significantly improves the performances due to its excellent electrical properties and deep quantum well, and the introduction of resistive material B$_{x} Ga_{1-x}$N as back barrier layer with 1% of boron concentration serves to improve the performances due to better confinement of (2DEG) two dimensional electron gas. With 20 nm gate length, the transistor demonstrates a maximum drain-source current (Ids) of 1.2 A/mm, a maximum transconductance (gm) of 425 mS mm$^{-1}$, a gate-leakage current of 3.10$^{-9}$ A, a cut-off frequency (Ft) of 850 GHz, and a maximum oscillation frequency (Fmax) of 1.5 THz.\",\"PeriodicalId\":401063,\"journal\":{\"name\":\"020 1st International Conference on Communications, Control Systems and Signal Processing (CCSSP)\",\"volume\":\"5 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2020-05-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"020 1st International Conference on Communications, Control Systems and Signal Processing (CCSSP)\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/CCSSP49278.2020.9151785\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"020 1st International Conference on Communications, Control Systems and Signal Processing (CCSSP)","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/CCSSP49278.2020.9151785","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
GaN/Inx Ga1-x N/B0.01 Ga0.99 N Double Heterojunction Field Effect Transistor DH-FET for electronics power application.
This paper aims to study a GaN/In$_{x} Ga_{1}xN/B_{0.01} Ga_{0.99}$ N Double Heterojunction Field Effect Transistor (DH-FET) by using SILVACO TCAD two and three dimensional device simulator. The structure is based on an undoped In$_{x} Ga_{1} x$ N as channel layer and an undopped back-barrier layer of B$_{x} Ga_{1-x}$N. The thickness of the channel layer has been fixed at 10 nm and we change the indium content in the alloy In$_{x} Ga_{1-x}$N of the channel layer, 10%, 25%, 50%, 75%, and 100% to get a channel layer only with nitride indium (InN). Some DC and AC performances of the transistor are simulated for each indium concentration.The increase of indium concentration in the In$_{x} Ga_{1-x}$N channel significantly improves the performances due to its excellent electrical properties and deep quantum well, and the introduction of resistive material B$_{x} Ga_{1-x}$N as back barrier layer with 1% of boron concentration serves to improve the performances due to better confinement of (2DEG) two dimensional electron gas. With 20 nm gate length, the transistor demonstrates a maximum drain-source current (Ids) of 1.2 A/mm, a maximum transconductance (gm) of 425 mS mm$^{-1}$, a gate-leakage current of 3.10$^{-9}$ A, a cut-off frequency (Ft) of 850 GHz, and a maximum oscillation frequency (Fmax) of 1.5 THz.