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Universal band gap modulation by radial deformation in semiconductor single-walled carbon nanotubes
https://iwate-u.repo.nii.ac.jp/records/9683
https://iwate-u.repo.nii.ac.jp/records/9683a14686fb-ea80-436e-b96d-391921bc461d
名前 / ファイル | ライセンス | アクション |
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Item type | 学術雑誌論文 / Journal Article(1) | |||||||||
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公開日 | 2009-01-09 | |||||||||
タイトル | ||||||||||
タイトル | Universal band gap modulation by radial deformation in semiconductor single-walled carbon nanotubes | |||||||||
キーワード | ||||||||||
主題Scheme | Other | |||||||||
主題 | ab initio calculations | |||||||||
キーワード | ||||||||||
主題Scheme | Other | |||||||||
主題 | carbon nanotubes | |||||||||
キーワード | ||||||||||
主題Scheme | Other | |||||||||
主題 | conduction bands | |||||||||
キーワード | ||||||||||
主題Scheme | Other | |||||||||
主題 | deformation | |||||||||
キーワード | ||||||||||
主題Scheme | Other | |||||||||
主題 | energy gap | |||||||||
キーワード | ||||||||||
主題Scheme | Other | |||||||||
主題 | semiconductor nanotubes | |||||||||
資源タイプ | ||||||||||
資源タイプ識別子 | http://purl.org/coar/resource_type/c_6501 | |||||||||
資源タイプ | journal article | |||||||||
著者 |
Nishidate, Kazume
× Nishidate, Kazume
× Hasegawa, Masayuki
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著者(機関) | ||||||||||
値 | Department of Electrical and Electronic Engineering | |||||||||
著者(機関) | ||||||||||
値 | Department of Materials Science and Engineering | |||||||||
登録日 | ||||||||||
日付 | 2009-01-09 | |||||||||
書誌情報 |
PHYSICAL REVIEW B 巻 78, 号 19, p. 195403-1-195403-6, 発行日 2008-01-01 |
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ISSN | ||||||||||
収録物識別子タイプ | ISSN | |||||||||
収録物識別子 | 1098-0121 | |||||||||
Abstract | ||||||||||
内容記述タイプ | Other | |||||||||
内容記述 | We report on a universal band gap modulation by radial deformation found for semiconductor single-walled carbon nanotubes (SWNTs). The plausible radial deformation of an individual SWNT under hydrostatic pressure is predicted using the method developed in the previous work [M. Hasegawa and K. Nishidate, Phys. Rev. B 74, 115401 (2006)]. It is found by ab initio electronic-structure calculations that the band gap of zigzag SWNTs is dictated by the shape of the high-curvature edge region of a deformed cross section perpendicular to the tube axis: If we let Rmin be an averaged curvature radius in that region, the band gap at the Γ point remains almost unchanged when Rmin≥3.2Å , and its closure occurs at Rmin≈2.4Å irrespective of tube size and cross-sectional shape as a whole. It is also confirmed that the band gap closure is accompanied by the concentration, in the high-curvature region, of the lowest conduction state at the Γ point. Possible implications of these results are discussed. | |||||||||
出版者 | ||||||||||
出版者 | American Physical Society | |||||||||
権利 | ||||||||||
権利情報 | ©2008 The American Physical Society | |||||||||
DOI | ||||||||||
関連タイプ | isIdenticalTo | |||||||||
識別子タイプ | DOI | |||||||||
関連識別子 | 10.1103/PhysRevB.78.195403 | |||||||||
著者版フラグ | ||||||||||
出版タイプ | VoR | |||||||||
出版タイプResource | http://purl.org/coar/version/c_970fb48d4fbd8a85 |