Synthesis of Polycrystalline Diamond Films in Abnormal Glow Discharge and their Properties; Journal of Physics: Conference Series; Vol. 652 : Gas Discharge Plasmas and Their Applications (GDP 2015)

Dades bibliogràfiques
Parent link:Journal of Physics: Conference Series
Vol. 652 : Gas Discharge Plasmas and Their Applications (GDP 2015).— 2015.— [012029, 6 p.]
Autor corporatiu: Национальный исследовательский Томский политехнический университет (ТПУ) Институт физики высоких технологий (ИФВТ) Лаборатория № 1, Национальный исследовательский Томский политехнический университет (ТПУ) Энергетический институт (ЭНИН) Кафедра электроснабжения промышленных предприятий (ЭПП)
Altres autors: Gaydaychuk A. V. Alexander Valerievich, Linnik S. A. Stepan Andreevich, Kabyshev A. V. Alexander Vasilievich, Konusov F. V. Fedor Valerievich, Remnev G. E. Gennady Efimovich
Sumari:Title screen
The optical and electrophysical properties of polycrystalline diamond films (PDF) deposited from the abnormal glow discharge have been studied. The dominating mechanisms of absorption and charge carrier transfer and the energy spectrum of the localized states (LS) of defects which determine the properties of the films have been specified. The parameters of the interband absorption and electrical conductivity are determined by the continuous energy distribution in the band gap (BG) of the states of defects of different nature. The absorption edge of the crystalline phase of the films is separated from the absorption zone determined by the electron transitions between LS defects. The width of BG is narrowed to 0.2-0.5 eV from the quantity typical to the diamond. An additional film absorption edge is formed in the energy interval 1.2-3.3 eV, where Urbach rule is fulfilled and the interband absorption is realized at direct transitions through the optical gap 1.1-1.5 eV. The average width of BG is 2.6-3.24 eV estimated within semiclassical interband model. The interaction of the parameters of the interband and exponential absorption is determined by the crystal lattice static disorder. The dominating n-type of the activation component of the electrical conductivity is complemented by the hopping mechanism with the participation of the localized states of the defects distributed near the Fermi level with a density 5.6•10{17}-2.1•10{21} eV{-1}•cm{-3}.
Режим доступа: по договору с организацией-держателем ресурса
Idioma:anglès
Publicat: 2015
Matèries:
Accés en línia:http://dx.doi.org/10.1088/1742-6596/652/1/012029
http://earchive.tpu.ru/handle/11683/18218
Format: Electrònic Capítol de llibre
KOHA link:https://koha.lib.tpu.ru/cgi-bin/koha/opac-detail.pl?biblionumber=644604

MARC

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200 1 |a Synthesis of Polycrystalline Diamond Films in Abnormal Glow Discharge and their Properties  |f A. V. Gaydaychuk [et al.] 
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300 |a Title screen 
320 |a [References: 19 tit.] 
330 |a The optical and electrophysical properties of polycrystalline diamond films (PDF) deposited from the abnormal glow discharge have been studied. The dominating mechanisms of absorption and charge carrier transfer and the energy spectrum of the localized states (LS) of defects which determine the properties of the films have been specified. The parameters of the interband absorption and electrical conductivity are determined by the continuous energy distribution in the band gap (BG) of the states of defects of different nature. The absorption edge of the crystalline phase of the films is separated from the absorption zone determined by the electron transitions between LS defects. The width of BG is narrowed to 0.2-0.5 eV from the quantity typical to the diamond. An additional film absorption edge is formed in the energy interval 1.2-3.3 eV, where Urbach rule is fulfilled and the interband absorption is realized at direct transitions through the optical gap 1.1-1.5 eV. The average width of BG is 2.6-3.24 eV estimated within semiclassical interband model. The interaction of the parameters of the interband and exponential absorption is determined by the crystal lattice static disorder. The dominating n-type of the activation component of the electrical conductivity is complemented by the hopping mechanism with the participation of the localized states of the defects distributed near the Fermi level with a density 5.6•10{17}-2.1•10{21} eV{-1}•cm{-3}. 
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701 1 |a Linnik  |b S. A.  |c physicist  |c Engineer-Researcher of Tomsk Polytechnic University  |f 1985-  |g Stepan Andreevich  |3 (RuTPU)RU\TPU\pers\32877  |9 16725 
701 1 |a Kabyshev  |b A. V.  |c specialist in the field of electric power engineering  |c Professor of Tomsk Polytechnic University, Doctor of physical and mathematical sciences  |f 1958-  |g Alexander Vasilievich  |3 (RuTPU)RU\TPU\pers\32572 
701 1 |a Konusov  |b F. V.  |c physicist  |c Lead Engineer of Tomsk Polytechnic University, Candidate of physical and mathematical sciences  |f 1958-  |g Fedor Valerievich  |y Tomsk  |3 (RuTPU)RU\TPU\pers\32570  |9 16491 
701 1 |a Remnev  |b G. E.  |c physicist  |c Professor of Tomsk Polytechnic University, Doctor of technical sciences  |f 1948-  |g Gennady Efimovich  |3 (RuTPU)RU\TPU\pers\31500 
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