{"title":"新型半导体Ti0.5Mg0.5N(001)","authors":"Baiwei Wang, D. Gall","doi":"10.1109/NANOTECH.2018.8653564","DOIUrl":null,"url":null,"abstract":"Ti<inf>0.5</inf>Mg<inf>0.5</inf>N has recently been predicted to be a semiconductor with a 1.3 eV band gap and promising properties for thermoelectric and plasmonic devices. As a first step towards experimental validation, epitaxial Ti<inf>0.5</inf>Mg<inf>0.5</inf>N(001) layers are deposited on MgO(001) by reactive magnetron co-sputtering from titanium and magnesium targets at 600 °C in pure N<inf>2</inf> atmospheres. X-ray diffraction ω-2θ scans, ω-rocking curves, φ-scans, and high resolution reciprocal space maps show that Ti<inf>0.5</inf>Mg<inf>0.5</inf>N alloys form a pseudobinary rocksalt structure and are single crystals with a cube-on-cube epitaxial relationship with the substrate: (001)<inf>TiMgN</inf> || (001)<inf>MgO</inf> and [100]<inf>TiMgN</inf> || [100]<inf>MgO</inf>. A 275-nm-thick Ti<inf>0.5</inf>Mg<inf>0.5</inf>N layer is fully relaxed and exhibits a 002 ω-rocking curve width Γ<inf>ω</inf> = 0.73°, while a 36-nm-thick layer is fully strained and has a Γ<inf>ω</inf> = 0.49°. These results indicate a thickness-dependent strain state which suggests a critical thickness for misfit dislocation nucleation and glide which is between 36 and 275 nm. A measured negative temperature coefficient of resistivity in combination with a low optical absorption coefficient of 0.25 × 10<sup>5</sup> cm<sup>−1</sup> for λ = 740 nm, and a vanishing density of states at the Fermi level measured by x-ray photoelectron spectroscopy support the prediction that Ti<inf>0.5</inf>Mg<inf>0.5</inf>N is a semiconductor.","PeriodicalId":292669,"journal":{"name":"2018 IEEE Nanotechnology Symposium (ANTS)","volume":"12 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2018-11-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"6","resultStr":"{\"title\":\"A new semiconductor: Ti0.5Mg0.5N(001)\",\"authors\":\"Baiwei Wang, D. Gall\",\"doi\":\"10.1109/NANOTECH.2018.8653564\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Ti<inf>0.5</inf>Mg<inf>0.5</inf>N has recently been predicted to be a semiconductor with a 1.3 eV band gap and promising properties for thermoelectric and plasmonic devices. As a first step towards experimental validation, epitaxial Ti<inf>0.5</inf>Mg<inf>0.5</inf>N(001) layers are deposited on MgO(001) by reactive magnetron co-sputtering from titanium and magnesium targets at 600 °C in pure N<inf>2</inf> atmospheres. X-ray diffraction ω-2θ scans, ω-rocking curves, φ-scans, and high resolution reciprocal space maps show that Ti<inf>0.5</inf>Mg<inf>0.5</inf>N alloys form a pseudobinary rocksalt structure and are single crystals with a cube-on-cube epitaxial relationship with the substrate: (001)<inf>TiMgN</inf> || (001)<inf>MgO</inf> and [100]<inf>TiMgN</inf> || [100]<inf>MgO</inf>. A 275-nm-thick Ti<inf>0.5</inf>Mg<inf>0.5</inf>N layer is fully relaxed and exhibits a 002 ω-rocking curve width Γ<inf>ω</inf> = 0.73°, while a 36-nm-thick layer is fully strained and has a Γ<inf>ω</inf> = 0.49°. These results indicate a thickness-dependent strain state which suggests a critical thickness for misfit dislocation nucleation and glide which is between 36 and 275 nm. A measured negative temperature coefficient of resistivity in combination with a low optical absorption coefficient of 0.25 × 10<sup>5</sup> cm<sup>−1</sup> for λ = 740 nm, and a vanishing density of states at the Fermi level measured by x-ray photoelectron spectroscopy support the prediction that Ti<inf>0.5</inf>Mg<inf>0.5</inf>N is a semiconductor.\",\"PeriodicalId\":292669,\"journal\":{\"name\":\"2018 IEEE Nanotechnology Symposium (ANTS)\",\"volume\":\"12 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2018-11-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"6\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"2018 IEEE Nanotechnology Symposium (ANTS)\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/NANOTECH.2018.8653564\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"2018 IEEE Nanotechnology Symposium (ANTS)","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/NANOTECH.2018.8653564","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Ti0.5Mg0.5N has recently been predicted to be a semiconductor with a 1.3 eV band gap and promising properties for thermoelectric and plasmonic devices. As a first step towards experimental validation, epitaxial Ti0.5Mg0.5N(001) layers are deposited on MgO(001) by reactive magnetron co-sputtering from titanium and magnesium targets at 600 °C in pure N2 atmospheres. X-ray diffraction ω-2θ scans, ω-rocking curves, φ-scans, and high resolution reciprocal space maps show that Ti0.5Mg0.5N alloys form a pseudobinary rocksalt structure and are single crystals with a cube-on-cube epitaxial relationship with the substrate: (001)TiMgN || (001)MgO and [100]TiMgN || [100]MgO. A 275-nm-thick Ti0.5Mg0.5N layer is fully relaxed and exhibits a 002 ω-rocking curve width Γω = 0.73°, while a 36-nm-thick layer is fully strained and has a Γω = 0.49°. These results indicate a thickness-dependent strain state which suggests a critical thickness for misfit dislocation nucleation and glide which is between 36 and 275 nm. A measured negative temperature coefficient of resistivity in combination with a low optical absorption coefficient of 0.25 × 105 cm−1 for λ = 740 nm, and a vanishing density of states at the Fermi level measured by x-ray photoelectron spectroscopy support the prediction that Ti0.5Mg0.5N is a semiconductor.