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Focusing on the area close to the Fermi level, a simple cubic lattice \u003cbr /\u003estructure is adopted instead of the real diamond one to simulate the various valence \u003cbr /\u003eband nature of BDD. This can simplify the problem without losing the key point. \u003cbr /\u003e For the phonon effect becomes significant just after the doping, we take into \u003cbr /\u003eaccount the electron-phonon (e-ph) coupling only at the doped sites. However, the \u003cbr /\u003ephonon effect is then not very noticeable after averaging all the sites, so we also \u003cbr /\u003ecalculate the spectrum of doped sites only, beside the whole system spectrum. From \u003cbr /\u003ethe classical Monte Carlo (MC) computation, the emergence of a clear Fermi edge is \u003cbr /\u003eseen. increasing the doping ratio, the impurity band expands upto the top of valence \u003cbr /\u003eband, and fills the small semiconductor gap gradually. Thus, the sample undergoes a \u003cbr /\u003esemiconductor-metal transition. Electrons can move freely from one impurity atom to \u003cbr /\u003eanother one through those intermediate carbon atoms. In quantum MC simulations, \u003cbr /\u003ethe lattice Green\u0027s function is calculated by the path-integral theory to reproduce the \u003cbr /\u003espectral function. From the whole system spectra, the phase transition is confirmed on \u003cbr /\u003ethe increase of the dopant concentration. The satellite structure is observed in the \u003cbr /\u003edoped sites spectrum, even within lightly doped sample. This structure has not been \u003cbr /\u003efound in classical MC cases, obviously coming from the phonon quantum character in \u003cbr /\u003ethe e-ph coupling. Increasing the coupling constant, a second phonon peak also \u003cbr /\u003epresents corresponding to the double-phonon, even multi-phonon scattering process. \u003cbr /\u003eBecause of the stronger coupling, a clear Fermi edge also appears although the doping \u003cbr /\u003erate is low. The co-existence of a Fermi edge and the step-like multi-phonon satellite \u003cbr /\u003estructure is reproduced completely, which can be interpreted from the two basic \u003cbr /\u003eproperties of electrons: itineracy and localization. \u003cbr /\u003e At the same time, our method, which can distinguish the spectra of different \u003cbr /\u003ecomponents in the material as we have done in calculating the spectra for the whole \u003cbr /\u003esystem and the doped sites only respectively, is very useful-to study the doped \u003cbr /\u003esystems, and to explain the resonant PES experiments. 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Photoemission Spectra Calculation of Boron-Doped Diamond using Quantum Monte Carlo Method
https://ir.soken.ac.jp/records/680
https://ir.soken.ac.jp/records/68083995575-a19a-4377-9b06-311d707443da
名前 / ファイル | ライセンス | アクション |
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Item type | 学位論文 / Thesis or Dissertation(1) | |||||
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公開日 | 2010-02-22 | |||||
タイトル | ||||||
タイトル | Photoemission Spectra Calculation of Boron-Doped Diamond using Quantum Monte Carlo Method | |||||
タイトル | ||||||
言語 | en | |||||
タイトル | Photoemission Spectra Calculation of Boron-Doped Diamond using Quantum Monte Carlo Method | |||||
言語 | ||||||
言語 | eng | |||||
資源タイプ | ||||||
資源タイプ識別子 | http://purl.org/coar/resource_type/c_46ec | |||||
資源タイプ | thesis | |||||
著者名 |
余, 継鋒
× 余, 継鋒 |
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フリガナ |
ユジファン
× ユジファン |
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著者 |
YU, Jifeng
× YU, Jifeng |
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学位授与機関 | ||||||
学位授与機関名 | 総合研究大学院大学 | |||||
学位名 | ||||||
学位名 | 博士(理学) | |||||
学位記番号 | ||||||
内容記述タイプ | Other | |||||
内容記述 | 総研大甲第1094号 | |||||
研究科 | ||||||
値 | 高エネルギー加速器科学研究科 | |||||
専攻 | ||||||
値 | 13 物質構造科学専攻 | |||||
学位授与年月日 | ||||||
学位授与年月日 | 2007-09-28 | |||||
学位授与年度 | ||||||
2007 | ||||||
要旨 | ||||||
内容記述タイプ | Other | |||||
内容記述 | In this thesis, we apply a new path-integral theory to the many impurities Holstein <br />model to calculate the photoemission spectra (PES) of a doped simple cubic lattice. <br />We mean to investigate the two intrinsic attributes of electrons: itineracy and <br />localization, which is able to clarify the co-existence of a Fermi edge and the step-like <br />multi-phonon structure, observed recently in the PES experiment of the boron-doped <br />diamond (BDD). Focusing on the area close to the Fermi level, a simple cubic lattice <br />structure is adopted instead of the real diamond one to simulate the various valence <br />band nature of BDD. This can simplify the problem without losing the key point. <br /> For the phonon effect becomes significant just after the doping, we take into <br />account the electron-phonon (e-ph) coupling only at the doped sites. However, the <br />phonon effect is then not very noticeable after averaging all the sites, so we also <br />calculate the spectrum of doped sites only, beside the whole system spectrum. From <br />the classical Monte Carlo (MC) computation, the emergence of a clear Fermi edge is <br />seen. increasing the doping ratio, the impurity band expands upto the top of valence <br />band, and fills the small semiconductor gap gradually. Thus, the sample undergoes a <br />semiconductor-metal transition. Electrons can move freely from one impurity atom to <br />another one through those intermediate carbon atoms. In quantum MC simulations, <br />the lattice Green's function is calculated by the path-integral theory to reproduce the <br />spectral function. From the whole system spectra, the phase transition is confirmed on <br />the increase of the dopant concentration. The satellite structure is observed in the <br />doped sites spectrum, even within lightly doped sample. This structure has not been <br />found in classical MC cases, obviously coming from the phonon quantum character in <br />the e-ph coupling. Increasing the coupling constant, a second phonon peak also <br />presents corresponding to the double-phonon, even multi-phonon scattering process. <br />Because of the stronger coupling, a clear Fermi edge also appears although the doping <br />rate is low. The co-existence of a Fermi edge and the step-like multi-phonon satellite <br />structure is reproduced completely, which can be interpreted from the two basic <br />properties of electrons: itineracy and localization. <br /> At the same time, our method, which can distinguish the spectra of different <br />components in the material as we have done in calculating the spectra for the whole <br />system and the doped sites only respectively, is very useful-to study the doped <br />systems, and to explain the resonant PES experiments. | |||||
所蔵 | ||||||
値 | 有 |