FRANTA, Daniel, Vilma BURŠÍKOVÁ, David NEČAS and Lenka ZAJÍČKOVÁ. Modeling of optical constants of diamond-like carbon. Diamond and Related Materials. New York: Elsevier, 2008, vol. 17, No 1, p. 705–708. ISSN 0925-9635.
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Basic information
Original name Modeling of optical constants of diamond-like carbon
Name in Czech Modelování optických konstant diamantu podobných vrstev
Authors FRANTA, Daniel (203 Czech Republic, guarantor, belonging to the institution), Vilma BURŠÍKOVÁ (203 Czech Republic, belonging to the institution), David NEČAS (203 Czech Republic, belonging to the institution) and Lenka ZAJÍČKOVÁ (203 Czech Republic, belonging to the institution).
Edition Diamond and Related Materials, New York, Elsevier, 2008, 0925-9635.
Other information
Original language English
Type of outcome Article in a journal
Field of Study 10302 Condensed matter physics
Country of publisher United States of America
Confidentiality degree is not subject to a state or trade secret
Impact factor Impact factor: 2.092
RIV identification code RIV/00216224:14310/08:00024371
Organization unit Faculty of Science
UT WoS 000256643300065
Keywords in English Diamon-like carbon; Amorphou hydrogenated carbon; Optical properties; Band structure
Tags Amorphou hydrogenated carbon, Band structure, Diamon-like carbon, Optical properties
Tags International impact, Reviewed
Changed by Changed by: doc. Mgr. Lenka Zajíčková, Ph.D., učo 1414. Changed: 27/3/2013 09:18.
Abstract
A new model of optical constants of diamond-like carbon parameterizing joint density of states (PJDOS) is introduced and compared with a previously published model based on the parameterization of density of states (PDOS). Both the models employ only six parameters: three parameters for pi-to-pi and three parameters for sigma-to-sigma transitions. These parameters have clear physical meaning. One describes the minimum energy needed for the band transition, i.e. band gap, the second is the maximum energy of transitions and the third is proportional to total density of corresponding electronic states. A certain disadvantage of PDOS model consists in the necessity of a numerical calculation. On the other hand the PJDOS model is analytical and, therefore, it can be implemented in a simple manner. The efficiency of both the models for study of DLC structure is demonstrated in several examples.
Abstract (in Czech)
A new model of optical constants of diamond-like carbon parameterizing joint density of states (PJDOS) is introduced and compared with a previously published model based on the parameterization of density of states (PDOS). Both the models employ only six parameters: three parameters for pi-to-pi and three parameters for sigma-to-sigma transitions. These parameters have clear physical meaning. One describes the minimum energy needed for the band transition, i.e. band gap, the second is the maximum energy of transitions and the third is proportional to total density of corresponding electronic states. A certain disadvantage of PDOS model consists in the necessity of a numerical calculation. On the other hand the PJDOS model is analytical and, therefore, it can be implemented in a simple manner. The efficiency of both the models for study of DLC structure is demonstrated in several examples.
Links
GA202/07/1669, research and development projectName: Depozice termomechanicky stabilních nanostrukturovaných diamantu-podobných tenkých vrstev ve dvojfrekvenčních kapacitních výbojích
Investor: Czech Science Foundation, Deposition of thermomehanically stable nanostructured diamond-like thin films in dual frequency capacitive discharges
KAN311610701, research and development projectName: Nanometrologie využívající metod rastrovací sondové mikroskopie
Investor: Academy of Sciences of the Czech Republic
MSM0021622411, plan (intention)Name: Studium a aplikace plazmochemických reakcí v neizotermickém nízkoteplotním plazmatu a jeho interakcí s povrchem pevných látek
Investor: Ministry of Education, Youth and Sports of the CR, Study and application of plasma chemical reactions in non-isothermic low temperature plasma and its interaction with solid surface
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