T. Kanazawa, K. Wakabayashi, H. Saito, R. Terao, Tomonori Tajima, S. Ikeda, Y. Miyamoto, K. Furuya
{"title":"亚微米InP/InGaAs复合沟道mosfet,选择性再生N+源极/漏极埋在沟道凹边","authors":"T. Kanazawa, K. Wakabayashi, H. Saito, R. Terao, Tomonori Tajima, S. Ikeda, Y. Miyamoto, K. Furuya","doi":"10.1109/ICIPRM.2010.5515922","DOIUrl":null,"url":null,"abstract":"We demonstrated a high-mobility InP 5 nm/InGaAs 12 nm composite channel MOSFET with MOVPE regrown n<sup>+</sup>-source/drain region for low series resistance and high source injection current. A gate dielectric was SiO<inf>2</inf> and thickness was 20 nm. A carrier density of regrown InGaAs source/drain layer was over 4 × 10<sup>19</sup> cm<sup>−3</sup>. In the measurement of submicron (= 150 nm) device, the drain current was 0.93 mA/µm at V<inf>g</inf> = 3 V, V<inf>d</inf> = 1 V and the peak transconductance was 0.53 mS/µm at V<inf>d</inf> = 0.65 V, respectively. The channel length dependence of transconductance indicated the good relativity.","PeriodicalId":197102,"journal":{"name":"2010 22nd International Conference on Indium Phosphide and Related Materials (IPRM)","volume":"15 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2010-07-23","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"2","resultStr":"{\"title\":\"Submicron InP/InGaAs composite channel MOSFETs with selectively regrown N+-source/drain buried in channel undercut\",\"authors\":\"T. Kanazawa, K. Wakabayashi, H. Saito, R. Terao, Tomonori Tajima, S. Ikeda, Y. Miyamoto, K. Furuya\",\"doi\":\"10.1109/ICIPRM.2010.5515922\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"We demonstrated a high-mobility InP 5 nm/InGaAs 12 nm composite channel MOSFET with MOVPE regrown n<sup>+</sup>-source/drain region for low series resistance and high source injection current. A gate dielectric was SiO<inf>2</inf> and thickness was 20 nm. A carrier density of regrown InGaAs source/drain layer was over 4 × 10<sup>19</sup> cm<sup>−3</sup>. In the measurement of submicron (= 150 nm) device, the drain current was 0.93 mA/µm at V<inf>g</inf> = 3 V, V<inf>d</inf> = 1 V and the peak transconductance was 0.53 mS/µm at V<inf>d</inf> = 0.65 V, respectively. The channel length dependence of transconductance indicated the good relativity.\",\"PeriodicalId\":197102,\"journal\":{\"name\":\"2010 22nd International Conference on Indium Phosphide and Related Materials (IPRM)\",\"volume\":\"15 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2010-07-23\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"2\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"2010 22nd International Conference on Indium Phosphide and Related Materials (IPRM)\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/ICIPRM.2010.5515922\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"2010 22nd International Conference on Indium Phosphide and Related Materials (IPRM)","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/ICIPRM.2010.5515922","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Submicron InP/InGaAs composite channel MOSFETs with selectively regrown N+-source/drain buried in channel undercut
We demonstrated a high-mobility InP 5 nm/InGaAs 12 nm composite channel MOSFET with MOVPE regrown n+-source/drain region for low series resistance and high source injection current. A gate dielectric was SiO2 and thickness was 20 nm. A carrier density of regrown InGaAs source/drain layer was over 4 × 1019 cm−3. In the measurement of submicron (= 150 nm) device, the drain current was 0.93 mA/µm at Vg = 3 V, Vd = 1 V and the peak transconductance was 0.53 mS/µm at Vd = 0.65 V, respectively. The channel length dependence of transconductance indicated the good relativity.