On the Origin of Light Emission in Silicon Rich Oxide Obtained by Low-Pressure Chemical Vapor Deposition

Silicon Rich Oxide (SRO) has been considered as a material to overcome the drawbacks of silicon to achieve optical functions. Various techniques can be used to produce it, including Low-Pressure Chemical Vapor Deposition (LPCVD). In this paper, a brief description of the studies carried out and disc...

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Detalhes bibliográficos
Autores: MARIANO ACEVES MIJARES, Roberto Stack Murphy Arteaga
Formato: artículo
Estado:Versión aceptada para publicación
Fecha de publicación:2012
País:México
Recursos:Instituto Nacional de Astrofísica, Óptica y Electrónica
Repositorio:Repositorio Institucional del INAOE
Idioma:inglés
OAI Identifier:oai:inaoe.repositorioinstitucional.mx:1009/2055
Acesso em linha:http://inaoe.repositorioinstitucional.mx/jspui/handle/1009/2055
Access Level:acceso abierto
Palavra-chave:info:eu-repo/classification/Inspec/Silicon Rich Oxide
info:eu-repo/classification/Inspec/Low-Pressure Chemical
info:eu-repo/classification/Inspec/LPCVD
info:eu-repo/classification/Inspec/Vapor Deposition
info:eu-repo/classification/cti/1
info:eu-repo/classification/cti/22
info:eu-repo/classification/cti/2203
Descrição
Resumo:Silicon Rich Oxide (SRO) has been considered as a material to overcome the drawbacks of silicon to achieve optical functions. Various techniques can be used to produce it, including Low-Pressure Chemical Vapor Deposition (LPCVD). In this paper, a brief description of the studies carried out and discussions of the results obtained on electro-, cathode-, and photoluminescence properties of SRO prepared by LPCVD and annealed at 1,100◦C are presented. The experimental results lead us to accept that SRO emission properties are due to oxidation state nanoagglomerates rather than to nanocrystals. The emission mechanism is similar to Donor-Acceptor decay in semiconductors, and a wide emission spectrum, from 450 to 850 nm, has been observed. The results show that emission is a function of both silicon excess in the film and excitation energy. As a result different color emissions can be obtained by selecting the suitable excitation energy.