{"title":"Ge1- xsnx和Ge1- xPbx合金电子结构演变的比较分析","authors":"C. Broderick, Edmond J. O’Halloran, E. O’Reilly","doi":"10.1109/NUSOD.2019.8806886","DOIUrl":null,"url":null,"abstract":"We present a comparative analysis of electronic structure evolution and the indirect- to direct-gap transition in Ge<inf>1−x</inf>(Sn,Pb)<inf>x</inf> group-IV semiconductor alloys. We present first principles disordered alloy electronic structure calculations for Ge<inf>1−x</inf>(Sn,Pb)<inf>x</inf> special quasi-random structures, and find a significantly larger band gap reduction in Ge<inf>1−x</inf>Pb<inf>x</inf> than in Ge<inf>1−x</inf>Sn<inf>x</inf> at fixed x. We calculate that Ge<inf>1−x</inf>Pb<inf>x</inf> becomes a direct gap semiconductor close to the composition (x ≈ 7%) at which it also becomes a zero-gap semiconductor. The indirect-to direct-gap transition in Ge<inf>1−x</inf>Sn<inf>x</inf> occurs over an extended composition range, also centered around 7%, and is driven by Sn-induced mixing of Ge Γ and L conduction states. The pronounced band mixing effects present in Ge<inf>1−x</inf>Sn<inf>x</inf> alloys will have significant implications for optical and transport properties.","PeriodicalId":369769,"journal":{"name":"2019 International Conference on Numerical Simulation of Optoelectronic Devices (NUSOD)","volume":"41 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2019-07-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"3","resultStr":"{\"title\":\"Comparative analysis of electronic structure evolution in Ge1-xSnx and Ge1−xPbx alloys\",\"authors\":\"C. Broderick, Edmond J. O’Halloran, E. O’Reilly\",\"doi\":\"10.1109/NUSOD.2019.8806886\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"We present a comparative analysis of electronic structure evolution and the indirect- to direct-gap transition in Ge<inf>1−x</inf>(Sn,Pb)<inf>x</inf> group-IV semiconductor alloys. We present first principles disordered alloy electronic structure calculations for Ge<inf>1−x</inf>(Sn,Pb)<inf>x</inf> special quasi-random structures, and find a significantly larger band gap reduction in Ge<inf>1−x</inf>Pb<inf>x</inf> than in Ge<inf>1−x</inf>Sn<inf>x</inf> at fixed x. We calculate that Ge<inf>1−x</inf>Pb<inf>x</inf> becomes a direct gap semiconductor close to the composition (x ≈ 7%) at which it also becomes a zero-gap semiconductor. The indirect-to direct-gap transition in Ge<inf>1−x</inf>Sn<inf>x</inf> occurs over an extended composition range, also centered around 7%, and is driven by Sn-induced mixing of Ge Γ and L conduction states. The pronounced band mixing effects present in Ge<inf>1−x</inf>Sn<inf>x</inf> alloys will have significant implications for optical and transport properties.\",\"PeriodicalId\":369769,\"journal\":{\"name\":\"2019 International Conference on Numerical Simulation of Optoelectronic Devices (NUSOD)\",\"volume\":\"41 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2019-07-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"3\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"2019 International Conference on Numerical Simulation of Optoelectronic Devices (NUSOD)\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/NUSOD.2019.8806886\",\"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 International Conference on Numerical Simulation of Optoelectronic Devices (NUSOD)","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/NUSOD.2019.8806886","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Comparative analysis of electronic structure evolution in Ge1-xSnx and Ge1−xPbx alloys
We present a comparative analysis of electronic structure evolution and the indirect- to direct-gap transition in Ge1−x(Sn,Pb)x group-IV semiconductor alloys. We present first principles disordered alloy electronic structure calculations for Ge1−x(Sn,Pb)x special quasi-random structures, and find a significantly larger band gap reduction in Ge1−xPbx than in Ge1−xSnx at fixed x. We calculate that Ge1−xPbx becomes a direct gap semiconductor close to the composition (x ≈ 7%) at which it also becomes a zero-gap semiconductor. The indirect-to direct-gap transition in Ge1−xSnx occurs over an extended composition range, also centered around 7%, and is driven by Sn-induced mixing of Ge Γ and L conduction states. The pronounced band mixing effects present in Ge1−xSnx alloys will have significant implications for optical and transport properties.