1990
DOI: 10.1063/1.345808
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Graphitic network models of ‘‘diamondlike’’ carbon

Abstract: We use simple arguments to fix the range of density of randomly distributed defects over which 1T electrons in a graphic sheet are strongly localized, but the underlying two-dimensional carbon network remains connected. This "defeated graphite" construct leads to simple structural models of both hydrogenated and unhydrogenated amorphous "diamondlike" carbon, which reproduce many important properties of those materials.

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Cited by 172 publications
(68 citation statements)
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“…We used the aromatic H/C ratio and aromatic+aliphatic H/C ratio, presented as two linear fits for the hydrogen poor (low E g ) regime (only soots). When both aromatic and aliphatic CH modes are included, our linear fit approaches the coefficient found for amorphous carbon in Tamor & Wu (1990). The shape of the symbols corresponds to those used in Fig.…”
Section: H/c Ratiossupporting
confidence: 52%
“…We used the aromatic H/C ratio and aromatic+aliphatic H/C ratio, presented as two linear fits for the hydrogen poor (low E g ) regime (only soots). When both aromatic and aliphatic CH modes are included, our linear fit approaches the coefficient found for amorphous carbon in Tamor & Wu (1990). The shape of the symbols corresponds to those used in Fig.…”
Section: H/c Ratiossupporting
confidence: 52%
“…Hence, until such time as the gaps have been filled we rely upon a recentlydeveloped set of optical properties for a large part of the a-C(:H) family parameter space (Jones 2012a,b,c). These optical properties were built ground-up using random covalent network (RCN) models (Phillips 1979;Döhler et al 1980;Thorpe 1983;Angus & Jansen 1988) and extensions thereof (extended RCN (eRCN) and Defective Graphite (DG) models, Tamor & Wu 1990;Jones 1990Jones , 2012a to construct a solid-state framework method to derive their structure and thence their complex indices of refraction. This approach determines the compositionand size-dependent optical properties of a-C(:H) materials (the optEC (s) and optEC (s) (a) datasets, Jones 2012a,b,c) based upon eRCN and DG modelling methods (Jones 1990(Jones , 2012a.…”
Section: Hydrogenated Amorphous Carbons A-c(:h)mentioning
confidence: 99%
“…Hydrogenated amorphous carbon materials, a-C(:H), are macroscopically-structured, contiguous network, solid-state materials comprised of only carbon and hydrogen atoms. The properties of a-C(:H) materials have been well-studied within both the physics and astrophysics communities (e.g., Phillips 1979;Döhler et al 1980;Thorpe 1983;Robertson 1986Robertson , 1988Robertson , 1991Robertson , 2001Robertson , 2002Robertson & O'Reilly 1987;Angus & Jansen 1988;Angus & Hayman 1988;Tamor & Wu 1990;Mennella et al 1995Mennella et al , 1996Mennella et al , 2003Ferrari & Robertson 2000Kassavetis et al 2007;Llamas-Jansa et al 2007;Mennella 2008;Gadallah et al 2011;Jones 2012a,b,c).…”
Section: Hydrogenated Amorphous Carbons A-c(:h)mentioning
confidence: 99%
“…For these truly amorphous materials it turns out that it is medium-range, rather than shortrange, order that determines the band gap (Robertson 1986). Laboratory studies of amorphous hydrocarbons show that there is a linear relationship between the band gap of these materials and their hydrocarbon content (Tamor & Wu 1990)…”
Section: The Optical Properties Of Hydrogenated Amorphous Carbonsmentioning
confidence: 99%