X. Gong, Ying Wu, Haiwen Xu, Kaizhen Han, L. Chua, W. Zou, T. Henry
{"title":"超低比接触电阻率金属/ p型GeSn触点","authors":"X. Gong, Ying Wu, Haiwen Xu, Kaizhen Han, L. Chua, W. Zou, T. Henry","doi":"10.23919/IWJT.2019.8802888","DOIUrl":null,"url":null,"abstract":"Contact resistance R c in the source/drain (S/D) regions of field-effect transistors (FETs) has increased significantly due to the shrinkage of contact area accompanied with the scaling of device dimensions in the past decades [1] . For the state-of-art transistor technology, the contact area is around 10×10 nm 2 [2] . R c , inversely proportional to the effective contact area, is the main parasitic resistance that limits the on-state current and switching speed of the device in the leading technology. To alleviate the impact of R c , an ultralow specific contact resistivity ρ c of less than 10 −9 Ω-cm 2 is required [3] .","PeriodicalId":441279,"journal":{"name":"2019 19th International Workshop on Junction Technology (IWJT)","volume":"120 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2019-06-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Metal/P-type GeSn Contacts with Ultra-low Specific Contact Resistivity\",\"authors\":\"X. Gong, Ying Wu, Haiwen Xu, Kaizhen Han, L. Chua, W. Zou, T. Henry\",\"doi\":\"10.23919/IWJT.2019.8802888\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Contact resistance R c in the source/drain (S/D) regions of field-effect transistors (FETs) has increased significantly due to the shrinkage of contact area accompanied with the scaling of device dimensions in the past decades [1] . For the state-of-art transistor technology, the contact area is around 10×10 nm 2 [2] . R c , inversely proportional to the effective contact area, is the main parasitic resistance that limits the on-state current and switching speed of the device in the leading technology. To alleviate the impact of R c , an ultralow specific contact resistivity ρ c of less than 10 −9 Ω-cm 2 is required [3] .\",\"PeriodicalId\":441279,\"journal\":{\"name\":\"2019 19th International Workshop on Junction Technology (IWJT)\",\"volume\":\"120 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2019-06-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"2019 19th International Workshop on Junction Technology (IWJT)\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.23919/IWJT.2019.8802888\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"2019 19th International Workshop on Junction Technology (IWJT)","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.23919/IWJT.2019.8802888","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Metal/P-type GeSn Contacts with Ultra-low Specific Contact Resistivity
Contact resistance R c in the source/drain (S/D) regions of field-effect transistors (FETs) has increased significantly due to the shrinkage of contact area accompanied with the scaling of device dimensions in the past decades [1] . For the state-of-art transistor technology, the contact area is around 10×10 nm 2 [2] . R c , inversely proportional to the effective contact area, is the main parasitic resistance that limits the on-state current and switching speed of the device in the leading technology. To alleviate the impact of R c , an ultralow specific contact resistivity ρ c of less than 10 −9 Ω-cm 2 is required [3] .