Lifetime of Shockley States on Metal Surfaces : Condensed Matter: Electronic Properties, etc.
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概要
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The lifetime of Shockley states on metal Surfaces is calculated under the assumption that the Coulomb interaction between electrons in Shockley states is mainly responsible for the finite lifetime of these states, and that the Coulonrb interaction would be screened by the bulk electrons. With single-particle wave functions of Shockley states, the Fourier expansion component of the screened Coulomb potential, V_s, is calculated, and the dependence of V_s on the lattice constant and the width of the projected band gap at the edge of the first Brillouin zone (Γ^^-) are investigated. A second-order perturbation calculation with respect to V_s is performed for the self-energy of a single electron in Shockley states, and then the lifetimes of these states on Cu(111) and Ag(111) surfaces are evaluated. Our results qualitatively agree with experimental results.
- 社団法人日本物理学会の論文
- 2001-01-15
著者
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NAKANISHI Hiroshi
Department of Precision Science and Technology and Applied Physics, Osaka University
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KASAI Hideaki
Department of Precision Science and Technology and Applied Physics, Osaka University
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Okiji A
Wakayama National Coll. Of Technol. Wakayama Jpn
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Okiji Ayao
Wakayama National College Of Technology
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Fukui A
Tokai Univ. Shizuoka Jpn
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Fukui Atsushi
Department Of Applied Physics Osaka University
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Kasai Hideaki
Department Of Applied Physics Osaka University
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FUKUl Atsushi
Department of Applied Physics,Osaka University
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Kasai Hideaki
Department Of Applied Physics Faculty Of Engineering Osaka University
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Nakanishi Hiroshi
Department Of Electronic Engineering Faculty Of Engineering Yamanashi University:(present Address) Sanken Electric Co. Ltd.
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Nakanishi Hiroshi
Department Of Biological Science And Technology Tokyo University Of Science
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Okiji Ayao
Department of Applied Physics, Osaka University
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Nakanishi Hiroshi
Department of Applied Physics, Graduate School of Engineering, Osaka University, Suita, Osaka 565-0871, Japan
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